From c5516ee40348504f830fa41e1baafc201c3f71fe Mon Sep 17 00:00:00 2001 From: Emmanuel Giner Date: Tue, 24 Mar 2020 15:26:32 +0100 Subject: [PATCH] removed useless files from revision --- Revised_Manuscript/.gitignore | 1 + Revised_Manuscript/Makefile | 51 - Revised_Manuscript/SI/srDFT_SC-SI.aux | 51 - Revised_Manuscript/SI/srDFT_SC-SI.bbl | 59 - Revised_Manuscript/SI/srDFT_SC-SI.blg | 67 - Revised_Manuscript/SI/srDFT_SC-SI.log | 2065 --- Revised_Manuscript/SI/srDFT_SC-SI.out | 8 - Revised_Manuscript/SI/srDFT_SC-SI.pdf | Bin 354627 -> 0 bytes Revised_Manuscript/SI/srDFT_SC-SINotes.bib | 2 - Revised_Manuscript/TODO | 3 - Revised_Manuscript/biblio.bib | 11864 ---------------- .../C2/DFT_avdzE_relat-eps-converted-to.pdf | Bin 13914 -> 0 bytes .../DFT_avdzE_relat_zoom-eps-converted-to.pdf | Bin 15036 -> 0 bytes .../C2/DFT_avtzE_relat-eps-converted-to.pdf | Bin 13890 -> 0 bytes .../DFT_avtzE_relat_zoom-eps-converted-to.pdf | Bin 15187 -> 0 bytes .../F2/DFT_vdzE_relat-eps-converted-to.pdf | Bin 14680 -> 0 bytes .../DFT_vdzE_relat_zoom-eps-converted-to.pdf | Bin 14838 -> 0 bytes .../F2/DFT_vqzE_relat-eps-converted-to.pdf | Bin 15046 -> 0 bytes .../DFT_vqzE_relat_zoom-eps-converted-to.pdf | Bin 14867 -> 0 bytes .../F2/DFT_vtzE_relat-eps-converted-to.pdf | Bin 14965 -> 0 bytes .../DFT_vtzE_relat_zoom-eps-converted-to.pdf | Bin 14866 -> 0 bytes .../H10/DFT_vdzE_relat-eps-converted-to.pdf | Bin 15030 -> 0 bytes .../DFT_vdzE_relat_zoom-eps-converted-to.pdf | Bin 16101 -> 0 bytes .../H10/DFT_vqzE_relat-eps-converted-to.pdf | Bin 15012 -> 0 bytes .../DFT_vqzE_relat_zoom-eps-converted-to.pdf | Bin 15865 -> 0 bytes .../H10/DFT_vtzE_relat-eps-converted-to.pdf | Bin 15058 -> 0 bytes .../DFT_vtzE_relat_zoom-eps-converted-to.pdf | Bin 15944 -> 0 bytes .../N2/DFT_avdzE_relat-eps-converted-to.pdf | Bin 14547 -> 0 bytes .../DFT_avdzE_relat_zoom-eps-converted-to.pdf | Bin 15388 -> 0 bytes .../N2/DFT_avtzE_relat-eps-converted-to.pdf | Bin 14571 -> 0 bytes .../DFT_avtzE_relat_zoom-eps-converted-to.pdf | Bin 15357 -> 0 bytes .../O2/DFT_avdzE_relat-eps-converted-to.pdf | Bin 14532 -> 0 bytes .../DFT_avdzE_relat_zoom-eps-converted-to.pdf | Bin 15461 -> 0 bytes Revised_Manuscript/srDFT_SC.aux | 306 - 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LaTeX info: "xparse/define-command" -. -. Defining command \vnabla with sig. '' on line 25. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \varE with sig. '' on line 29. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ordersymbol with sig. '' on line 30. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \lparen with sig. '' on line 31. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \rparen with sig. '' on line 32. -................................................. -................................................. -. 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LaTeX info: "xparse/redefine-command" -. -. Redefining command \cos with sig. '' on line 310. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \tan with sig. '' on line 311. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \csc with sig. '' on line 312. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \sec with sig. '' on line 313. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \cot with sig. '' on line 314. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \arcsin with sig. '' on line 316. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \arccos with sig. '' on line 317. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \arctan with sig. '' on line 318. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \arccsc with sig. '' on line 320. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \arcsec with sig. '' on line 322. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \arccot with sig. '' on line 324. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \asin with sig. '' on line 327. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \acos with sig. '' on line 329. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \atan with sig. '' on line 331. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \acsc with sig. '' on line 333. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \asec with sig. '' on line 335. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \acot with sig. '' on line 337. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \sinh with sig. '' on line 339. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \cosh with sig. '' on line 340. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \tanh with sig. '' on line 341. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \csch with sig. '' on line 343. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \sech with sig. '' on line 345. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \coth with sig. '' on line 346. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \exp with sig. '' on line 348. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \log with sig. '' on line 349. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \ln with sig. '' on line 350. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \det with sig. '' on line 351. -................................................. -................................................. -. LaTeX info: "xparse/redefine-command" -. -. Redefining command \Pr with sig. '' on line 352. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \tr with sig. '' on line 353. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \Tr with sig. '' on line 354. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \Res with sig. '' on line 355. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qqtext with sig. ' s m ' on line 377. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qq with sig. '' on line 378. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qcomma with sig. '' on line 380. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qc with sig. '' on line 381. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qif with sig. 's' on line 383. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qthen with sig. 's' on line 384. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qelse with sig. 's' on line 385. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qotherwise with sig. 's' on line 386. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qunless with sig. 's' on line 387. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qgiven with sig. 's' on line 388. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qusing with sig. 's' on line 389. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qassume with sig. 's' on line 390. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qsince with sig. 's' on line 391. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qlet with sig. 's' on line 392. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qfor with sig. 's' on line 393. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qall with sig. 's' on line 394. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qeven with sig. 's' on line 395. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qodd with sig. 's' on line 396. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qinteger with sig. 's' on line 397. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qand with sig. 's' on line 398. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qor with sig. 's' on line 399. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qas with sig. 's' on line 400. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qin with sig. 's' on line 401. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qcc with sig. 's' on line 402. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \differential with sig. ' o g d() ' on line 415. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dd with sig. '' on line 416. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \derivative with sig. ' s o m g d() ' on line 435. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dv with sig. '' on line 436. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \partialderivative with sig. ' s o m g g d() ' on line 460. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pderivative with sig. '' on line 461. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pdv with sig. '' on line 462. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \variation with sig. ' o g d() ' on line 474. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \var with sig. '' on line 475. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \functionalderivative with sig. ' s o m g d() ' on line -. 494. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \fderivative with sig. '' on line 495. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \fdv with sig. '' on line 496. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \bra with sig. ' s m t\ket s g ' on line 526. -................................................. -************************************************* -* LaTeX warning: "xparse/not-single-char" -* -* Argument delimiter '\ket ' for the command '\bra' should be a single -* character. -************************************************* -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ket with sig. ' s m ' on line 533. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \innerproduct with sig. ' s m g ' on line 548. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \braket with sig. '' on line 549. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ip with sig. '' on line 550. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \outerproduct with sig. ' s m g ' on line 565. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dyad with sig. '' on line 566. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \op with sig. '' on line 567. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ketbra with sig. '' on line 568. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \expectationvalue with sig. ' s s m g ' on line 587. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \expval with sig. '' on line 588. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ev with sig. '' on line 589. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \vev with sig. ' m ' on line 590. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \matrixelement with sig. ' s s m m m ' on line 601. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \matrixel with sig. '' on line 602. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \mel with sig. '' on line 603. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \identitymatrix with sig. 'm' on line 633. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \imat with sig. '' on line 634. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \xmatrix with sig. ' s m m m ' on line 659. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \xmat with sig. '' on line 660. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \zeromatrix with sig. ' m g ' on line 662. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \zmat with sig. '' on line 663. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \paulixmatrix with sig. '' on line 665. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pauliymatrix with sig. '' on line 666. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \paulizmatrix with sig. '' on line 667. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \paulimatrix with sig. 'm' on line 678. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pmat with sig. '' on line 679. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \diagonalmatrix with sig. 'O{} >{\SplitList {,}}m ' on line -. 681. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \@dmat with sig. 'mmggggggg' on line 714. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dmat with sig. '' on line 715. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \antidiagonalmatrix with sig. 'O{} >{\SplitList {,}}m ' on -. line 717. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \@admat with sig. 'mmggggggg' on line 750. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \admat with sig. '' on line 751. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \flatfrac with sig. ' m m ' on line 754. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \homework with sig. '' on line 764. -................................................. -) (/usr/share/texlive/texmf-dist/tex/latex/mhchem/mhchem.sty -Package: mhchem 2017/07/24 v4.07 for typesetting chemical formulae - -(/usr/share/texlive/texmf-dist/tex/latex/l3packages/l3keys2e/l3keys2e.sty -Package: l3keys2e 2018/02/21 LaTeX2e option processing using LaTeX3 keys -) -(/usr/share/texlive/texmf-dist/tex/latex/tools/calc.sty -Package: calc 2014/10/28 v4.3 Infix arithmetic (KKT,FJ) -\calc@Acount=\count199 -\calc@Bcount=\count266 -\calc@Adimen=\dimen148 -\calc@Bdimen=\dimen149 -\calc@Askip=\skip60 -\calc@Bskip=\skip61 -LaTeX Info: Redefining \setlength on input line 80. -LaTeX Info: Redefining \addtolength on input line 81. -\calc@Ccount=\count267 -\calc@Cskip=\skip62 -) -(/usr/share/texlive/texmf-dist/tex/latex/chemgreek/chemgreek.sty -Package: chemgreek 2016/12/20 v1.1 interfaceforuprightgreeklettersforuseinchemi -stry (CN) -\l__chemgreek_tmpa_int=\count268 -\g__chemgreek_tmpa_int=\count269 -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \newchemgreekmapping with sig. 'O{}mm' on line 336. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \renewchemgreekmapping with sig. 'O{}mm' on line 339. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \declarechemgreekmapping with sig. 'O{}mm' on line 342. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \newchemgreekmappingalias with sig. 'mm' on line 347. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \renewchemgreekmappingalias with sig. 'mm' on line 350. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \declarechemgreekmappingalias with sig. 'mm' on line 353. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \changechemgreeksymbol with sig. 'mmmm' on line 383. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \chemgreekmappingsymbol with sig. 'mm' on line 477. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \activatechemgreekmapping with sig. 'sm' on line 486. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \selectchemgreekmapping with sig. 'm' on line 491. -................................................. -) -\l__mhchem_ce_distanceFromLastComma_int=\count270 -\__mhchem_arrow_extPgfLength_skip=\skip63 -\mhchem@minispace@tmp=\skip64 -\mhchem@minibackspace@tmp=\skip65 -\mhchem@bondwidth=\skip66 -\mhchem@bondheight=\skip67 -\mhchem@smallbondwidth@tmpA=\skip68 -\mhchem@smallbondwidth@tmpB=\skip69 -\mhchem@smallbondwidth=\skip70 -\mhchem@bondtmp@minussidebearingleft=\skip71 -\mhchem@bondtmp@minussidebearingright=\skip72 -\l__mhchem_option_version_int=\count271 -\mhchem@option@minusmathsidebearingleft=\dimen150 -\mhchem@option@minusmathsidebearingright=\dimen151 -\mhchem@option@minustextsidebearingleft=\dimen152 -\mhchem@option@minustextsidebearingright=\dimen153 - - -Package mhchem Warning: You did not specify a 'version' option for the mhchem -(mhchem) package. Please write \usepackage[version=4]{mhchem} -(mhchem) in your preamble (or any lower number for -(mhchem) compatibility mode), because you might get slightly -(mhchem) different output with the same input in future versions -. - -) (/usr/share/texlive/texmf-dist/tex/latex/tools/xspace.sty -Package: xspace 2014/10/28 v1.13 Space after command names (DPC,MH) -) -(/usr/share/texlive/texmf-dist/tex/latex/psnfss/mathpazo.sty -Package: mathpazo 2005/04/12 PSNFSS-v9.2a Palatino w/ Pazo Math (D.Puga, WaS) -\symupright=\mathgroup9 -) -(/usr/share/texlive/texmf-dist/tex/latex/libertine/libertine.sty -Package: libertine 2018/01/03 (Bob Tennent) Supports Libertine and Biolinum fon -ts for all LaTeX engines. - -(/usr/share/texlive/texmf-dist/tex/generic/ifxetex/ifxetex.sty -Package: ifxetex 2010/09/12 v0.6 Provides ifxetex conditional -) -(/usr/share/texlive/texmf-dist/tex/generic/oberdiek/ifluatex.sty -Package: ifluatex 2016/05/16 v1.4 Provides the ifluatex switch (HO) -Package ifluatex Info: LuaTeX not detected. -) -(/usr/share/texlive/texmf-dist/tex/latex/xkeyval/xkeyval.sty -Package: xkeyval 2014/12/03 v2.7a package option processing (HA) - 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LaTeX info: "xparse/define-command" -. -. Defining command \vnabla with sig. '' on line 25. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \varE with sig. '' on line 29. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ordersymbol with sig. '' on line 30. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \lparen with sig. '' on line 31. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \rparen with sig. '' on line 32. -................................................. -................................................. -. 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LaTeX info: "xparse/define-command" -. -. Defining command \qty with sig. '' on line 63. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pqty with sig. ' l m ' on line 64. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \bqty with sig. ' l m ' on line 65. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \Bqty with sig. ' l m ' on line 66. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \vqty with sig. ' l m ' on line 67. -................................................. -................................................. -. 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'm' on line 105. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \sPmqty with sig. 'm' on line 106. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \sbmqty with sig. 'm' on line 107. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \svmqty with sig. 'm' on line 108. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \smallmatrixquantity with sig. ' s g o d() d|| ' on line -. 133. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. 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's' on line 397. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qand with sig. 's' on line 398. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qor with sig. 's' on line 399. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qas with sig. 's' on line 400. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qin with sig. 's' on line 401. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \qcc with sig. 's' on line 402. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \differential with sig. ' o g d() ' on line 415. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dd with sig. '' on line 416. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \derivative with sig. ' s o m g d() ' on line 435. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dv with sig. '' on line 436. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \partialderivative with sig. ' s o m g g d() ' on line 460. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pderivative with sig. '' on line 461. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pdv with sig. '' on line 462. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \variation with sig. ' o g d() ' on line 474. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \var with sig. '' on line 475. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \functionalderivative with sig. ' s o m g d() ' on line -. 494. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \fderivative with sig. '' on line 495. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \fdv with sig. '' on line 496. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \bra with sig. ' s m t\ket s g ' on line 526. -................................................. -************************************************* -* LaTeX warning: "xparse/not-single-char" -* -* Argument delimiter '\ket ' for the command '\bra' should be a single -* character. -************************************************* -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ket with sig. ' s m ' on line 533. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \innerproduct with sig. ' s m g ' on line 548. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \braket with sig. '' on line 549. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ip with sig. '' on line 550. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \outerproduct with sig. ' s m g ' on line 565. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dyad with sig. '' on line 566. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \op with sig. '' on line 567. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ketbra with sig. '' on line 568. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \expectationvalue with sig. ' s s m g ' on line 587. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \expval with sig. '' on line 588. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \ev with sig. '' on line 589. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \vev with sig. ' m ' on line 590. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \matrixelement with sig. ' s s m m m ' on line 601. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \matrixel with sig. '' on line 602. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \mel with sig. '' on line 603. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \identitymatrix with sig. 'm' on line 633. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \imat with sig. '' on line 634. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \xmatrix with sig. ' s m m m ' on line 659. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \xmat with sig. '' on line 660. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \zeromatrix with sig. ' m g ' on line 662. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \zmat with sig. '' on line 663. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \paulixmatrix with sig. '' on line 665. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pauliymatrix with sig. '' on line 666. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \paulizmatrix with sig. '' on line 667. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \paulimatrix with sig. 'm' on line 678. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \pmat with sig. '' on line 679. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \diagonalmatrix with sig. 'O{} >{\SplitList {,}}m ' on line -. 681. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \@dmat with sig. 'mmggggggg' on line 714. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \dmat with sig. '' on line 715. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \antidiagonalmatrix with sig. 'O{} >{\SplitList {,}}m ' on -. line 717. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \@admat with sig. 'mmggggggg' on line 750. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \admat with sig. '' on line 751. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \flatfrac with sig. ' m m ' on line 754. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \homework with sig. '' on line 764. -................................................. -) (/usr/share/texlive/texmf-dist/tex/latex/mhchem/mhchem.sty -Package: mhchem 2017/07/24 v4.07 for typesetting chemical formulae - -(/usr/share/texlive/texmf-dist/tex/latex/l3packages/l3keys2e/l3keys2e.sty -Package: l3keys2e 2018/02/21 LaTeX2e option processing using LaTeX3 keys -) -(/usr/share/texlive/texmf-dist/tex/latex/tools/calc.sty -Package: calc 2014/10/28 v4.3 Infix arithmetic (KKT,FJ) -\calc@Acount=\count199 -\calc@Bcount=\count266 -\calc@Adimen=\dimen148 -\calc@Bdimen=\dimen149 -\calc@Askip=\skip60 -\calc@Bskip=\skip61 -LaTeX Info: Redefining \setlength on input line 80. -LaTeX Info: Redefining \addtolength on input line 81. -\calc@Ccount=\count267 -\calc@Cskip=\skip62 -) -(/usr/share/texlive/texmf-dist/tex/latex/chemgreek/chemgreek.sty -Package: chemgreek 2016/12/20 v1.1 interfaceforuprightgreeklettersforuseinchemi -stry (CN) -\l__chemgreek_tmpa_int=\count268 -\g__chemgreek_tmpa_int=\count269 -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \newchemgreekmapping with sig. 'O{}mm' on line 336. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \renewchemgreekmapping with sig. 'O{}mm' on line 339. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \declarechemgreekmapping with sig. 'O{}mm' on line 342. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \newchemgreekmappingalias with sig. 'mm' on line 347. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \renewchemgreekmappingalias with sig. 'mm' on line 350. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \declarechemgreekmappingalias with sig. 'mm' on line 353. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \changechemgreeksymbol with sig. 'mmmm' on line 383. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \chemgreekmappingsymbol with sig. 'mm' on line 477. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \activatechemgreekmapping with sig. 'sm' on line 486. -................................................. -................................................. -. LaTeX info: "xparse/define-command" -. -. Defining command \selectchemgreekmapping with sig. 'm' on line 491. -................................................. -) -\l__mhchem_ce_distanceFromLastComma_int=\count270 -\__mhchem_arrow_extPgfLength_skip=\skip63 -\mhchem@minispace@tmp=\skip64 -\mhchem@minibackspace@tmp=\skip65 -\mhchem@bondwidth=\skip66 -\mhchem@bondheight=\skip67 -\mhchem@smallbondwidth@tmpA=\skip68 -\mhchem@smallbondwidth@tmpB=\skip69 -\mhchem@smallbondwidth=\skip70 -\mhchem@bondtmp@minussidebearingleft=\skip71 -\mhchem@bondtmp@minussidebearingright=\skip72 -\l__mhchem_option_version_int=\count271 -\mhchem@option@minusmathsidebearingleft=\dimen150 -\mhchem@option@minusmathsidebearingright=\dimen151 -\mhchem@option@minustextsidebearingleft=\dimen152 -\mhchem@option@minustextsidebearingright=\dimen153 - - -Package mhchem Warning: You did not specify a 'version' option for the mhchem -(mhchem) package. Please write \usepackage[version=4]{mhchem} -(mhchem) in your preamble (or any lower number for -(mhchem) compatibility mode), because you might get slightly -(mhchem) different output with the same input in future versions -. - -) (/usr/share/texlive/texmf-dist/tex/latex/tools/xspace.sty -Package: xspace 2014/10/28 v1.13 Space after command names (DPC,MH) -) -(/usr/share/texlive/texmf-dist/tex/latex/subfigure/subfigure.sty -Package: subfigure 2002/03/15 v2.1.5 subfigure package -\subfigtopskip=\skip73 -\subfigcapskip=\skip74 -\subfigcaptopadj=\dimen154 -\subfigbottomskip=\skip75 -\subfigcapmargin=\dimen155 -\subfiglabelskip=\skip76 -\c@subfigure=\count272 -\c@lofdepth=\count273 -\c@subtable=\count274 -\c@lotdepth=\count275 - -**************************************** -* Local config file subfigure.cfg used * -**************************************** -(/usr/share/texlive/texmf-dist/tex/latex/subfigure/subfigure.cfg) -\subfig@top=\skip77 -\subfig@bottom=\skip78 -) -(/usr/share/texlive/texmf-dist/tex/latex/base/inputenc.sty -Package: inputenc 2015/03/17 v1.2c Input encoding file -\inpenc@prehook=\toks24 -\inpenc@posthook=\toks25 - -(/usr/share/texlive/texmf-dist/tex/latex/base/utf8.def -File: utf8.def 2017/01/28 v1.1t UTF-8 support for inputenc -Now handling font encoding OML ... -... no UTF-8 mapping file for font encoding OML -Now handling font encoding T1 ... -... processing UTF-8 mapping file for font encoding T1 - -(/usr/share/texlive/texmf-dist/tex/latex/base/t1enc.dfu -File: t1enc.dfu 2017/01/28 v1.1t UTF-8 support for inputenc - defining Unicode char U+00A0 (decimal 160) - defining Unicode char U+00A1 (decimal 161) - defining Unicode char U+00A3 (decimal 163) - defining Unicode char U+00AB (decimal 171) - defining Unicode char U+00AD (decimal 173) - defining Unicode char U+00BB (decimal 187) - defining Unicode char U+00BF (decimal 191) - defining Unicode char U+00C0 (decimal 192) - defining Unicode char U+00C1 (decimal 193) - defining Unicode char U+00C2 (decimal 194) - defining Unicode char U+00C3 (decimal 195) - defining Unicode char U+00C4 (decimal 196) - defining Unicode char U+00C5 (decimal 197) - defining Unicode char U+00C6 (decimal 198) - defining Unicode char U+00C7 (decimal 199) - defining Unicode char U+00C8 (decimal 200) - defining Unicode char U+00C9 (decimal 201) - defining Unicode char U+00CA (decimal 202) - defining Unicode char U+00CB (decimal 203) - defining Unicode char U+00CC (decimal 204) - defining Unicode char U+00CD (decimal 205) - defining Unicode char U+00CE (decimal 206) - defining Unicode char U+00CF (decimal 207) - defining Unicode char U+00D0 (decimal 208) - defining Unicode char U+00D1 (decimal 209) - defining Unicode char U+00D2 (decimal 210) - defining Unicode char U+00D3 (decimal 211) - defining Unicode char U+00D4 (decimal 212) - defining Unicode char U+00D5 (decimal 213) - defining Unicode char U+00D6 (decimal 214) - defining Unicode char U+00D8 (decimal 216) - defining Unicode char U+00D9 (decimal 217) - defining Unicode char U+00DA (decimal 218) - defining Unicode char U+00DB (decimal 219) - defining Unicode char U+00DC (decimal 220) - defining Unicode char U+00DD (decimal 221) - defining Unicode char U+00DE (decimal 222) - defining Unicode char U+00DF (decimal 223) - defining Unicode char U+00E0 (decimal 224) - defining Unicode char U+00E1 (decimal 225) - defining Unicode char U+00E2 (decimal 226) - defining Unicode char U+00E3 (decimal 227) - defining Unicode char U+00E4 (decimal 228) - defining Unicode char U+00E5 (decimal 229) - defining Unicode char U+00E6 (decimal 230) - defining Unicode char U+00E7 (decimal 231) - defining Unicode char U+00E8 (decimal 232) - defining Unicode char U+00E9 (decimal 233) - defining Unicode char U+00EA (decimal 234) - defining Unicode char U+00EB (decimal 235) - defining Unicode char U+00EC (decimal 236) - defining Unicode char U+00ED (decimal 237) - defining Unicode char U+00EE (decimal 238) - defining Unicode char U+00EF (decimal 239) - defining Unicode char U+00F0 (decimal 240) - defining Unicode char U+00F1 (decimal 241) - defining Unicode char U+00F2 (decimal 242) - defining Unicode char U+00F3 (decimal 243) - defining Unicode char U+00F4 (decimal 244) - defining Unicode char U+00F5 (decimal 245) - defining Unicode char U+00F6 (decimal 246) - defining Unicode char U+00F8 (decimal 248) - defining Unicode char U+00F9 (decimal 249) - defining Unicode char U+00FA (decimal 250) - defining Unicode char U+00FB (decimal 251) - defining Unicode char U+00FC (decimal 252) - defining Unicode char U+00FD (decimal 253) - defining Unicode char U+00FE (decimal 254) - defining Unicode char U+00FF (decimal 255) - defining Unicode char U+0100 (decimal 256) - defining Unicode char U+0101 (decimal 257) - defining Unicode char U+0102 (decimal 258) - defining Unicode char U+0103 (decimal 259) - defining Unicode char U+0104 (decimal 260) - defining Unicode char U+0105 (decimal 261) - defining Unicode char U+0106 (decimal 262) - defining Unicode char U+0107 (decimal 263) - defining Unicode char U+0108 (decimal 264) - defining Unicode char U+0109 (decimal 265) - defining Unicode char U+010A (decimal 266) - defining Unicode char U+010B (decimal 267) - defining Unicode char U+010C (decimal 268) - defining Unicode char U+010D (decimal 269) - defining Unicode char U+010E (decimal 270) - defining Unicode char U+010F (decimal 271) - defining Unicode char U+0110 (decimal 272) - defining Unicode char U+0111 (decimal 273) - defining Unicode char U+0112 (decimal 274) - defining Unicode char U+0113 (decimal 275) - defining Unicode char U+0114 (decimal 276) - defining Unicode char U+0115 (decimal 277) - defining Unicode char U+0116 (decimal 278) - defining Unicode char U+0117 (decimal 279) - defining Unicode char U+0118 (decimal 280) - defining Unicode char U+0119 (decimal 281) - defining Unicode char U+011A (decimal 282) - defining Unicode char U+011B (decimal 283) - defining Unicode char U+011C (decimal 284) - defining Unicode char U+011D (decimal 285) - defining Unicode char U+011E (decimal 286) - defining Unicode char U+011F (decimal 287) - defining Unicode char U+0120 (decimal 288) - defining Unicode char U+0121 (decimal 289) - defining Unicode char U+0122 (decimal 290) - defining Unicode char U+0123 (decimal 291) - defining Unicode char U+0124 (decimal 292) - defining Unicode char U+0125 (decimal 293) - defining Unicode char U+0128 (decimal 296) - defining Unicode char U+0129 (decimal 297) - defining Unicode char U+012A (decimal 298) - defining Unicode char U+012B (decimal 299) - defining Unicode char U+012C (decimal 300) - defining Unicode char U+012D (decimal 301) - defining Unicode char U+012E (decimal 302) - defining Unicode char U+012F (decimal 303) - defining Unicode char U+0130 (decimal 304) - defining Unicode char U+0131 (decimal 305) - defining Unicode char U+0132 (decimal 306) - defining Unicode char U+0133 (decimal 307) - defining Unicode char U+0134 (decimal 308) - defining Unicode char U+0135 (decimal 309) - defining Unicode char U+0136 (decimal 310) - defining Unicode char U+0137 (decimal 311) - defining Unicode char U+0139 (decimal 313) - defining Unicode char U+013A (decimal 314) - defining Unicode char U+013B (decimal 315) - defining Unicode char U+013C (decimal 316) - defining Unicode char U+013D (decimal 317) - defining Unicode char U+013E (decimal 318) - defining Unicode char U+0141 (decimal 321) - defining Unicode char U+0142 (decimal 322) - defining Unicode char U+0143 (decimal 323) - defining Unicode char U+0144 (decimal 324) - defining Unicode char U+0145 (decimal 325) - defining Unicode char U+0146 (decimal 326) - defining Unicode char U+0147 (decimal 327) - defining Unicode char U+0148 (decimal 328) - defining Unicode char U+014A (decimal 330) - defining Unicode char U+014B (decimal 331) - defining Unicode char U+014C (decimal 332) - defining Unicode char U+014D (decimal 333) - defining Unicode char U+014E (decimal 334) - defining Unicode char U+014F (decimal 335) - defining Unicode char U+0150 (decimal 336) - defining Unicode char U+0151 (decimal 337) - defining Unicode char U+0152 (decimal 338) - defining Unicode char U+0153 (decimal 339) - defining Unicode char U+0154 (decimal 340) - defining Unicode char U+0155 (decimal 341) - defining Unicode char U+0156 (decimal 342) - defining Unicode char U+0157 (decimal 343) - defining Unicode char U+0158 (decimal 344) - defining Unicode char U+0159 (decimal 345) - defining Unicode char U+015A (decimal 346) - defining Unicode char U+015B (decimal 347) - defining Unicode char U+015C (decimal 348) - defining Unicode char U+015D (decimal 349) - defining Unicode char U+015E (decimal 350) - defining Unicode char U+015F (decimal 351) - defining Unicode char U+0160 (decimal 352) - defining Unicode char U+0161 (decimal 353) - defining Unicode char U+0162 (decimal 354) - defining Unicode char U+0163 (decimal 355) - defining Unicode char U+0164 (decimal 356) - defining Unicode char U+0165 (decimal 357) - defining Unicode char U+0168 (decimal 360) - defining Unicode char U+0169 (decimal 361) - defining Unicode char U+016A (decimal 362) - defining Unicode char U+016B (decimal 363) - defining Unicode char U+016C (decimal 364) - defining Unicode char U+016D (decimal 365) - defining Unicode char U+016E (decimal 366) - defining Unicode char U+016F (decimal 367) - defining Unicode char U+0170 (decimal 368) - defining Unicode char U+0171 (decimal 369) - defining Unicode char U+0172 (decimal 370) - defining Unicode char U+0173 (decimal 371) - defining Unicode char U+0174 (decimal 372) - defining Unicode char U+0175 (decimal 373) - defining Unicode char U+0176 (decimal 374) - defining Unicode char U+0177 (decimal 375) - defining Unicode char U+0178 (decimal 376) - defining Unicode char U+0179 (decimal 377) - defining Unicode char U+017A (decimal 378) - defining Unicode char U+017B (decimal 379) - defining Unicode char U+017C (decimal 380) - defining Unicode char U+017D (decimal 381) - defining Unicode char U+017E (decimal 382) - defining Unicode char U+01CD (decimal 461) - defining Unicode char U+01CE (decimal 462) - defining Unicode char U+01CF (decimal 463) - defining Unicode char U+01D0 (decimal 464) - defining Unicode char U+01D1 (decimal 465) - defining Unicode char U+01D2 (decimal 466) - defining Unicode char U+01D3 (decimal 467) - defining Unicode char U+01D4 (decimal 468) - defining Unicode char U+01E2 (decimal 482) - defining Unicode char U+01E3 (decimal 483) - defining Unicode char U+01E6 (decimal 486) - defining Unicode char U+01E7 (decimal 487) - defining Unicode char U+01E8 (decimal 488) - defining Unicode char U+01E9 (decimal 489) - defining Unicode char U+01EA (decimal 490) - defining Unicode char U+01EB (decimal 491) - defining Unicode char U+01F0 (decimal 496) - defining Unicode char U+01F4 (decimal 500) - defining Unicode char U+01F5 (decimal 501) - defining Unicode char U+0218 (decimal 536) - defining Unicode char U+0219 (decimal 537) - defining Unicode char U+021A (decimal 538) - defining Unicode char U+021B (decimal 539) - defining Unicode char U+0232 (decimal 562) - defining Unicode char U+0233 (decimal 563) - defining Unicode char U+1E02 (decimal 7682) - defining Unicode char U+1E03 (decimal 7683) - defining Unicode char U+200C (decimal 8204) - defining Unicode char U+2010 (decimal 8208) - defining Unicode char U+2011 (decimal 8209) - defining Unicode char U+2012 (decimal 8210) - defining Unicode char U+2013 (decimal 8211) - defining Unicode char U+2014 (decimal 8212) - defining Unicode char U+2015 (decimal 8213) - defining Unicode char U+2018 (decimal 8216) - defining Unicode char U+2019 (decimal 8217) - defining Unicode char U+201A (decimal 8218) - defining Unicode char U+201C (decimal 8220) - defining Unicode char U+201D (decimal 8221) - defining Unicode char U+201E (decimal 8222) - defining Unicode char U+2030 (decimal 8240) - defining Unicode char U+2031 (decimal 8241) - defining Unicode char U+2039 (decimal 8249) - defining Unicode char U+203A (decimal 8250) - defining Unicode char U+2423 (decimal 9251) - defining Unicode char U+1E20 (decimal 7712) - defining Unicode char U+1E21 (decimal 7713) -) -Now handling font encoding OT1 ... -... processing UTF-8 mapping file for font encoding OT1 - -(/usr/share/texlive/texmf-dist/tex/latex/base/ot1enc.dfu -File: ot1enc.dfu 2017/01/28 v1.1t UTF-8 support for inputenc - defining Unicode char U+00A0 (decimal 160) - defining Unicode char U+00A1 (decimal 161) - defining Unicode char U+00A3 (decimal 163) - defining Unicode char U+00AD (decimal 173) - defining Unicode char U+00B8 (decimal 184) - defining Unicode char U+00BF (decimal 191) - defining Unicode char U+00C5 (decimal 197) - defining Unicode char U+00C6 (decimal 198) - defining Unicode char U+00D8 (decimal 216) - defining Unicode char U+00DF (decimal 223) - defining Unicode char U+00E6 (decimal 230) - defining Unicode char U+00EC (decimal 236) - defining Unicode char U+00ED 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M. Barca and P.-F. Loos, [][]J. Chem. Phys. \T1/txr/b -x/n/8 147\T1/txr/m/n/8 (+20) , 024103 (2017)[][], - [] - -[14]) [15] -Package atveryend Info: Empty hook `AfterLastShipout' on input line 947. - (./srDFT_SC.aux) -Package atveryend Info: Executing hook `AtVeryEndDocument' on input line 947. -Package atveryend Info: Executing hook `AtEndAfterFileList' on input line 947. -Package rerunfilecheck Info: File `srDFT_SC.out' has not changed. -(rerunfilecheck) Checksum: 4B6311C7B61AB256A1DDF014715C94D2;2220. - ) -Here is how much of TeX's memory you used: - 22569 strings out of 494310 - 382433 string characters out of 6167045 - 540167 words of memory out of 5000000 - 25019 multiletter control sequences out of 15000+600000 - 643732 words of font info for 539 fonts, out of 8000000 for 9000 - 309 hyphenation exceptions out of 8191 - 39i,16n,56p,10380b,708s stack positions out of 5000i,500n,10000p,200000b,80000s -{/usr/share/texlive/texmf-dist/fonts/enc/dvips/base/8r.enc} -Output written on srDFT_SC.pdf (15 pages, 415131 bytes). -PDF statistics: - 907 PDF objects out of 1000 (max. 8388607) - 823 compressed objects within 9 object streams - 217 named destinations out of 1000 (max. 500000) - 76595 words of extra memory for PDF output out of 89155 (max. 10000000) - diff --git a/Revised_Manuscript/srDFT_SC.out b/Revised_Manuscript/srDFT_SC.out deleted file mode 100644 index b3d317c..0000000 --- a/Revised_Manuscript/srDFT_SC.out +++ /dev/null @@ -1,27 +0,0 @@ -\BOOKMARK [0][-]{section*.2}{A basis-set error correction based on density-functional theory for strongly correlated molecular systems}{}% 2 -\BOOKMARK [1][-]{section*.1}{Abstract}{section*.2}% 1 -\BOOKMARK [1][-]{section*.3}{Introduction}{section*.2}% 3 -\BOOKMARK [1][-]{section*.4}{Theory}{section*.2}% 4 -\BOOKMARK [2][-]{section*.5}{Basic theory}{section*.4}% 5 -\BOOKMARK [2][-]{section*.6}{Effective interaction in a finite basis}{section*.4}% 6 -\BOOKMARK [2][-]{section*.7}{Local range-separation function}{section*.4}% 7 -\BOOKMARK [3][-]{section*.8}{General definition}{section*.7}% 8 -\BOOKMARK [3][-]{section*.9}{Frozen-core approximation}{section*.7}% 9 -\BOOKMARK [2][-]{section*.10}{General form of the complementary functional}{section*.4}% 10 -\BOOKMARK [3][-]{section*.11}{Generic approximate form}{section*.10}% 11 -\BOOKMARK [3][-]{section*.12}{Two limits where the complementary functional vanishes}{section*.10}% 12 -\BOOKMARK [2][-]{section*.13}{Requirements on the complementary functional for strong correlation}{section*.4}% 13 -\BOOKMARK [3][-]{section*.14}{Spin-multiplet degeneracy}{section*.13}% 14 -\BOOKMARK [3][-]{section*.15}{Size consistency}{section*.13}% 15 -\BOOKMARK [2][-]{section*.16}{Actual approximations used for the complementary functional}{section*.4}% 16 -\BOOKMARK [1][-]{section*.17}{Results}{section*.2}% 17 -\BOOKMARK [2][-]{section*.18}{Computational details}{section*.17}% 18 -\BOOKMARK [2][-]{section*.19}{H10 chain}{section*.17}% 19 -\BOOKMARK [2][-]{section*.20}{Dissociation of diatomics}{section*.17}% 20 -\BOOKMARK [1][-]{section*.21}{Conclusion}{section*.2}% 21 -\BOOKMARK [1][-]{section*.22}{Size consistency of the basis-set correction}{section*.2}% 22 -\BOOKMARK [2][-]{section*.23}{Sufficient condition for size consistency}{section*.22}% 23 -\BOOKMARK [2][-]{section*.24}{Intensivity of the on-top pair density and the local range-separation function}{section*.22}% 24 -\BOOKMARK [1][-]{section*.25}{Computational cost of the basis-set correction for a CASSCF wave function}{section*.2}% 25 -\BOOKMARK [2][-]{section*.26}{Computation of the on-top pair density}{section*.25}% 26 -\BOOKMARK [2][-]{section*.27}{Computation of the local range-separation function}{section*.25}% 27 diff --git a/Revised_Manuscript/srDFT_SC.tex.bak b/Revised_Manuscript/srDFT_SC.tex.bak deleted file mode 100644 index b18d819..0000000 --- a/Revised_Manuscript/srDFT_SC.tex.bak +++ /dev/null @@ -1,779 +0,0 @@ -\documentclass[aip,jcp,reprint,noshowkeys,superscriptaddress]{revtex4-1} -\usepackage{graphicx,dcolumn,bm,xcolor,microtype,multirow,amsmath,amssymb,amsfonts,physics,mhchem,xspace} - 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- - -\newcommand{\ex}[4]{$^{#1}#2_{#3}^{#4}$} -\newcommand{\ra}{\rightarrow} -\newcommand{\De}{D_\text{e}} - -% MODEL -\newcommand{\model}[0]{\mathcal{Y}} - -% densities -\newcommand{\denmodel}[0]{\den_{\model}^\Bas} -\newcommand{\denmodelr}[0]{\den_{\model}^\Bas ({\bf r})} -\newcommand{\denfci}[0]{\den_{\psifci}} -\newcommand{\denFCI}[0]{\den^{\Bas}_{\text{FCI}}} -\newcommand{\denhf}[0]{\den_{\text{HF}}^\Bas} -\newcommand{\denrfci}[0]{\denr_{\psifci}} -\newcommand{\dencipsir}[0]{{n}_{\text{CIPSI}}^\Bas({\bf r})} -\newcommand{\dencipsi}[0]{{n}_{\text{CIPSI}}^\Bas} -\newcommand{\den}[0]{{n}} -\newcommand{\denval}[0]{{n}^{\text{val}}} -\newcommand{\denr}[0]{{n}({\bf r})} -\newcommand{\onedmval}[0]{\rho_{ij,\sigma}^{\text{val}}} - -% wave functions -\newcommand{\psifci}[0]{\Psi^{\Bas}_{\text{FCI}}} -\newcommand{\psimu}[0]{\Psi^{\mu}} -% operators -\newcommand{\weeopbasis}[0]{\hat{W}_{\text{ee}}^\Bas} -\newcommand{\kinop}[0]{\hat{T}} - -\newcommand{\weeopbasisval}[0]{\hat{W}_{\text{ee}}^{\Basval}} -\newcommand{\weeop}[0]{\hat{W}_{\text{ee}}} - - -% units -\newcommand{\IneV}[1]{#1 eV} -\newcommand{\InAU}[1]{#1 a.u.} -\newcommand{\InAA}[1]{#1 \AA} - - -% methods -\newcommand{\UEG}{\text{UEG}} -\newcommand{\LDA}{\text{LDA}} -\newcommand{\PBE}{\text{PBE}} -\newcommand{\FCI}{\text{FCI}} -\newcommand{\CCSDT}{\text{CCSD(T)}} -\newcommand{\lr}{\text{lr}} -\newcommand{\sr}{\text{sr}} - -\newcommand{\Nel}{N} -\newcommand{\V}[2]{V_{#1}^{#2}} - - -\newcommand{\n}[2]{n_{#1}^{#2}} -\newcommand{\E}[2]{E_{#1}^{#2}} -\newcommand{\bE}[2]{\Bar{E}_{#1}^{#2}} -\newcommand{\bEc}[1]{\Bar{E}_\text{c}^{#1}} -\newcommand{\e}[2]{\varepsilon_{#1}^{#2}} -\newcommand{\be}[2]{\Bar{\varepsilon}_{#1}^{#2}} -\newcommand{\bec}[1]{\Bar{e}^{#1}} -\newcommand{\wf}[2]{\Psi_{#1}^{#2}} -\newcommand{\W}[2]{W_{#1}^{#2}} -\newcommand{\w}[2]{w_{#1}^{#2}} -\newcommand{\hn}[2]{\Hat{n}_{#1}^{#2}} -\newcommand{\rsmu}[2]{\mu_{#1}^{#2}} -\newcommand{\SO}[2]{\phi_{#1}(\br{#2})} - -\newcommand{\modX}{\text{X}} -\newcommand{\modY}{\text{Y}} - -% basis sets -\newcommand{\setdenbasis}{\mathcal{N}_{\Bas}} -\newcommand{\Bas}{\mathcal{B}} -\newcommand{\basis}{\mathcal{B}} -\newcommand{\Basval}{\mathcal{B}_\text{val}} -\newcommand{\Val}{\mathcal{V}} -\newcommand{\Cor}{\mathcal{C}} - -% operators -\renewcommand{\d}{\text{d}} -\newcommand{\hT}{\Hat{T}} -\newcommand{\hWee}[1]{\Hat{W}_\text{ee}^{#1}} -\newcommand{\f}[2]{f_{#1}^{#2}} -\newcommand{\Gam}[2]{\Gamma_{#1}^{#2}} -\newcommand{\isEquivTo}[1]{\underset{#1}{\sim}} - -% coordinates -\newcommand{\br}[1]{{\mathbf{r}_{#1}}} -\newcommand{\bx}[1]{\mathbf{x}_{#1}} -\newcommand{\dbr}[1]{d\br{#1}} -\newcommand{\PBEspin}{PBEspin} -\newcommand{\PBEueg}{PBE-UEG-{$\tilde{\zeta}$}} - -\newcommand{\LCT}{Laboratoire de Chimie Th\'eorique (UMR 7616), Sorbonne Universit\'e, CNRS, Paris, France} -\newcommand{\ISCD}{Institut des Sciences du Calcul et des Donn\'ees, Sorbonne Universit\'e, Paris, France} -\newcommand{\LCPQ}{Laboratoire de Chimie et Physique Quantiques (UMR 5626), Universit\'e de Toulouse, CNRS, UPS, France} -\newcommand{\IUF}{Institut Universitaire de France, Paris, France} - - -\begin{document} - -\title{A density-based basis-set correction for strong correlation} - -\author{Emmanuel Giner} -\email{emmanuel.giner@lct.jussieu.fr} -\affiliation{\LCT} -\author{Barth\'el\'emy Pradines} -\affiliation{\LCT} -\affiliation{\ISCD} -\author{Anthony Scemama} -\affiliation{\LCPQ} -\author{Pierre-Fran\c{c}ois Loos} -\email{loos@irsamc.ups-tlse.fr} -\affiliation{\LCPQ} -\author{Julien Toulouse} -\email{toulouse@lct.jussieu.fr} -\affiliation{\LCT} -\affiliation{\IUF} - - -\begin{abstract} -We extend to strongly correlated systems the recently introduced basis-set correction based on density-functional theory (DFT) [E. Giner \textit{et al.}, J. Chem. Phys. \textbf{149}, 194301 (2018)]. This basis-set correction relies on a mapping between wave-function calculations in a finite basis set and range-separated DFT (RSDFT) through the definition of an effective non-divergent interaction corresponding to the Coulomb electron-electron interaction projected in the finite basis set, allowing one to use RSDFT-type complementary functionals to recover the dominant part of the short-range correlation effects missing in a finite basis set. Using as test cases the potential energy curves of the H$_{10}$, C$_2$, N$_2$, O$_2$, and F$_2$ molecules up to the dissociation limit, we systematically explore different approximations for the complementary functionals which are suited to describe strong-correlation regimes and which fulfill two very desirable properties: $S_z$ invariance and size consistency. Specifically, we investigate the dependence of the functionals on different flavours of on-top pair densities and spin polarizations. An important result is that the explicit dependence on the on-top pair density allows one to completely remove the dependence on any form of spin polarization without any significant loss of accuracy. -In the general context of multiconfigurational DFT, this finding shows that one can avoid the effective spin polarization whose mathematical definition is rather \textit{ad hoc} and which can become complex valued. Quantitatively, we show that the basis-set correction reaches chemical accuracy on atomization energies with triple-zeta quality basis sets for most of the systems studied. Also, the present basis-set correction provides smooth curves along the whole potential energy curves. -%We study the potential energy surfaces (PES) of the H$_{10}$, C$_2$, N$_2$, O$_2$, and F$_2$ molecules up to the dissociation limit using increasing basis sets at near full configuration interaction (FCI) level with and without the present basis-set correction. -\end{abstract} - -\maketitle - -%%%%%%%%%%%%%%%%%%%%%%%% -\section{Introduction} -%%%%%%%%%%%%%%%%%%%%%%%% -The general goal of quantum chemistry is to provide reliable theoretical tools to explore the rich area of chemistry. More specifically, developments in quantum chemistry primarily aim at accurately computing the electronic structure of molecular systems, but despite intense developments, no definitive solution to this problem has been found. The theoretical challenge to tackle belongs to the quantum many-body problem, due the intrinsic quantum nature of the electrons and the Coulomb repulsion between them. This so-called electronic correlation problem corresponds to finding a solution to the Schr\"odinger equation for a $N$-electron system, and two main roads have emerged to approximate this solution: wave-function theory (WFT)~\cite{Pop-RMP-99} and density-functional theory (DFT)~\cite{Koh-RMP-99}. Although both WFT and DFT spring from the same Schr\"odinger equation, they rely on very different formalisms, as the former deals with the complicated $N$-electron wave function whereas the latter focuses on the much simpler one-electron density. In its Kohn-Sham (KS) formulation~\cite{KohSha-PR-65}, the computational cost of DFT is very appealing since it is a simple mean-field procedure. Therefore, although continued efforts have been done to reduce the computational cost of WFT, DFT still remains the workhorse of quantum chemistry. - -The difficulty of obtaining a reliable theoretical description of a given chemical system can be roughly categorized by the strength of the electronic correlation appearing in its electronic structure. The so-called weakly correlated systems, such as closed-shell organic molecules near their equilibrium geometries, are typically dominated by correlation effects which do not affect the qualitative mean-field picture of the system. These weak correlation effects can be either short range(near the electron-electron coalescence point) or long range (London dispersion interactions). The theoretical description of weakly correlated systems is one of the most concrete achievement of quantum chemistry, and the main remaining issue for these systems is to push the limit of the size of the chemical systems that can be treated. The case of the so-called strongly correlated systems, which are ubiquitous in chemistry, is much more problematic as they exhibit a much more complex electronic structure. For example, transition metal complexes, low-spin open-shell systems, covalent bond breaking situations have all in common that they cannot be even qualitatively described by a single electronic configuration. It is now clear that the usual semilocal density-functional approximations of KS DFT fail to accurately describe these situations and WFT is king for the treatment of strongly correlated systems. - -In practice WFT uses a finite one-particle basis set (here denoted as $\basis$) to project the Schr\"odinger equation. The exact solution within the basis set is then provided by full configuration interaction (FCI) which consists in a linear-algebra problem with a dimension scaling exponentially with the system size. Due to this exponential growth of the FCI computational cost, introducing approximations is necessary, with at least two difficulties for strongly correlated systems: i) the qualitative description of the wave function is determined by a primary set of electronic configurations (whose size can scale exponentially in many cases) among which near degeneracies and/or strong interactions appear in the Hamiltonian matrix; ii) the quantitative description of the system requires to also account for weak correlation effects which involve many other electronic configurations with typically much smaller weights in the wave function. Addressing these two objectives is a rather complicated task for a given approximate WFT method, especially if one adds the requirement of satisfying formal properties, such as spin-multiplet degeneracy and size consistency. - -%To tackle this complicated problem, many methods have been proposed and an exhaustive review of the zoology of methods for strong correlation goes beyond the scope and purpose of this article. - -%To tackle this problem, many WFT methods have emerged which can be categorized in two branches: the single-reference (SR) -%and multi-reference (MR) methods. -%The SR methods rely on a single electronic configuration as a zeroth-order wave function, typically Hartree-Fock (HF). -%Then the electron correlation is introduced by increasing the rank of multiple hole-particle excitations, -%preferably treated in a coupled-cluster (CC) fashion for the sake of compactness of the wave function and extensivity of the computed energies. -%The advantage of these approaches rely on the rather straightforward way to improve the level of accuracy, -%which consists in increasing the rank of the excitation operators used to generate the CC wave function. -%Despite its appealing elegant simplicity, the computational cost of the CC methods increase drastically with the rank of the excitation -%operators, even if promising alternative approaches have been proposed using stochastic techniques\cite{Thom-PRL-10,ScoTho-JCP-17,SpeNeuVigFraTho-JCP-18,DeuEmiShePie-PRL-17,DeuEmiMagShePie-JCP-18,DeuEmiYumShePie-JCP-19} or symmetry-broken approaches\cite{QiuHenZhaScu-JCP-17,QiuHenZhaScu-JCP-18,GomHenScu-JCP-19}. -%In the MR approaches, the zeroth order wave function consists in a linear combination of Slater determinants which are supposed to concentrate most of strong interactions and near degeneracies inherent in the structure of the Hamiltonian for a strongly correlated system. The usual approach to build such a zeroth-order wave function is to perform a complete active space self consistent field (CASSCF) whose variational property prevent any divergence, and which can provide extensive energies. Of course, the choice of the active space is rather a subtle art and the CASSCF results might strongly depend on the level of chemical/physical knowledge of the user. -%On top of this zeroth-order wave function, weak correlation is introduced by the addition of other configurations through either configuration interaction\cite{WerKno-JCP-88,KnoWer-CPL-88} (MRCI) or perturbation theory (MRPT) and even coupled cluster (MRCC), which have their strengths and weaknesses, -%The advantage of MRCI approaches rely essentially in their simple linear parametrisation for the wave function together with the variational property of their energies, whose inherent drawback is the lack of size extensivity of their energies unless reaching the FCI limit. On the other hand, MRPT and MRCC can provide extensive energies but to the price of rather complicated formalisms, and these approaches might be subject to divergences and/or convergence problems due to the non linearity of the parametrisation for MRCC or a too poor choice of the zeroth-order Hamiltonian. -%A natural alternative is to combine MRCI and MRPT, which falls in the category of selected CI (SCI) which goes back to the late 60's and who has received a revival of interest and applications during the last decade \cite{BenErn-PhysRev-1969,WhiHac-JCP-1969,HurMalRan-1973,EvaDauMal-ChemPhys-83,Cim-JCP-1985,Cim-JCC-1987,IllRubRic-JCP-88,PovRubIll-TCA-92,BunCarRam-JCP-06,AbrSheDav-CPL-05,MusEngels-JCC-06,BytRue-CP-09,GinSceCaf-CJC-13,CafGinScemRam-JCTC-14,GinSceCaf-JCP-15,CafAplGinScem-arxiv-16,CafAplGinSce-JCP-16,SchEva-JCP-16,LiuHofJCTC-16,HolUmrSha-JCP-17,ShaHolJeaAlaUmr-JCTC-17,HolUmrSha-JCP-17,SchEva-JCTC-17,PerCle-JCP-17,OhtJun-JCP-17,Zim-JCP-17,LiOttHolShaUmr-JCP-2018,ChiHolOttUmrShaZim-JPCA-18,SceBenJacCafLoo-JCP-18,LooSceBloGarCafJac-JCTC-18,GarSceGinCaffLoo-JCP-18,SceGarCafLoo-JCTC-18,GarGinMalSce-JCP-16,LooBogSceCafJac-JCTC-19}. -%Among the SCI algorithms, the CI perturbatively selected iteratively (CIPSI) can be considered as a pioneer. The main idea of the CIPSI and other related SCI algorithms is to iteratively select the most important Slater determinants thanks to perturbation theory in order to build a MRCI zeroth-order wave function which automatically concentrate the strongly interacting part of the wave function. On top of this MRCI zeroth-order wave function, a rather simple MRPT approach is used to recover the missing weak correlation and the process is iterated until reaching a given convergence criterion. It is important to notice that in the SCI algorithms, neither the SCI or the MRPT are size extensive \textit{per se}, but the extensivity property is almost recovered by approaching the FCI limit. -%When the SCI are affordable, their clear advantage are that they provide near FCI wave functions and energies, whatever the level of knowledge of the user on the specific physical/chemical problem considered. The drawback of SCI is certainly their \textit{intrinsic} exponential scaling due to their linear parametrisation. Nevertheless, such an exponential scaling is lowered by the smart selection of the zeroth-order wave function together with the MRPT calculation. - -Beside the difficulties of accurately describing the molecular electronic structure within a given basis set, a crucial limitation of WFT methods is the slow convergence of the energies and properties with respect to the size of the basis set. As initially shown by the seminal work of Hylleraas\cite{Hyl-ZP-29} and further developed by Kutzelnigg and coworkers~\textit{et al.}\cite{Kut-TCA-85,KutKlo-JCP-91, NogKut-JCP-94}, the main convergence problem originates from the divergence of the Coulomb electron-electron interaction at the coalescence point, which induces a discontinuity in the first derivative of the exact wave function (the so-called electron-electron cusp). Describing such a discontinuity with an incomplete one-electron basis set is impossible and, as a consequence, the convergence of the computed energies and properties can be strongly affected. To attenuate this problem, extrapolation techniques have been developed, either based on a partial-wave expansion analysis~\cite{HelKloKocNog-JCP-97,HalHelJorKloKocOlsWil-CPL-98}, or more recently based on perturbative arguments\cite{IrmHulGru-arxiv-19}. A more rigorous approach to tackle the basis-set convergence problem is provided by the so-called R12 and F12 explicitly correlated methods\cite{Ten-TCA-12,TenNog-WIREs-12,HatKloKohTew-CR-12, KonBisVal-CR-12, GruHirOhnTen-JCP-17, MaWer-WIREs-18} which introduce a geminal function explicitly depending on the interelectronic distances ensuring the correct cusp condition in the wave function, and lead to a much faster convergence of the correlation energies than usual WFT methods. For instance, using the explicitly correlated version of coupled cluster with singles, doubles, and perturbative triples (CCSD(T)) in a triple-$\zeta$ quality basis set is equivalent to using a quintuple-$\zeta$ quality basis set with the usual CCSD(T) method\cite{TewKloNeiHat-PCCP-07}, although a computational overhead is introduced by the auxiliary basis set needed to compute the three- and four-electron integrals involved in F12 theory. In addition to the computational cost, a possible drawback of F12 theory is its rather complex formalism which requires non-trivial developments for adapting it to a new method. For strongly correlated systems, several multi-reference methods have been extended to explicitly correlation (see for instance Ref.~\onlinecite{Ten-CPL-07,ShiWer-JCP-10,TorKniWer-JCP-11,DemStanMatTenPitNog-PCCP-12,GuoSivValNee-JCP-17}), including approaches based on the so-called universal F12 theory which are potentially applicable to any electronic-structure computational methods~\cite{TorVal-JCP-09,KonVal-JCP-11,HauMaoMukKlo-CPL-12,BooCleAlaTew-JCP-12}. - -An alternative way to improve the convergence towards the complete-basis-set (CBS) limit is to treat the short-range correlation effects within DFT and to use WFT methods to deal only with the long-range and/or strong-correlation effects. A rigorous approach achieving this mixing of DFT and WFT is range-separated DFT (RSDFT) (see Ref.~\onlinecite{TouColSav-PRA-04} and references therein) which relies on a splitting of the Coulomb electron-electron interaction in terms of the interelectronic distance thanks to a range-separation parameter $\mu$. The advantage of this approach is at least two-fold: i) the DFT part deals primarily with the short-range part of the Coulomb interaction, and consequently the usual semilocal density-functional approximations are more accurate than for standard KS DFT; ii) the WFT part deals only with a smooth non-divergent interaction, and consequently the wave function has no electron-electron cusp\cite{GorSav-PRA-06} and the basis-set convergence is much faster\cite{FraMusLupTou-JCP-15}. A number of approximate RSDFT schemes have been developed involving single-reference \cite{AngGerSavTou-PRA-05, GolWerSto-PCCP-05, TouGerJanSavAng-PRL-09,JanHenScu-JCP-09, TouZhuSavJanAng-JCP-11, MusReiAngTou-JCP-15,KalTou-JCP-18,KalMusTou-JCP-19} or multi-reference \cite{LeiStoWerSav-CPL-97, FroTouJen-JCP-07, FroCimJen-PRA-10, HedKneKieJenRei-JCP-15, HedTouJen-JCP-18, FerGinTou-JCP-18} WFT methods. Nevertheless, there are still some open issues in RSDFT, such as remaining fractional-charge and fractional-spin errors in the short-range density functionals~\cite{MusTou-MP-17} or the dependence of the quality of the results on the value of the range-separation parameter $\mu$. -% which can be seen as an empirical parameter. - -Building on the development of RSDFT, a possible solution to the basis-set convergence problem has been recently proposed by some of the present authors~\cite{GinPraFerAssSavTou-JCP-18} where RSDFT functionals are used to recover only the correlation effects outside a given basis set. The key point here is to realize that a wave function developed in an incomplete basis set is cuspless and could also come from a Hamiltonian with a non divergent electron-electron interaction. Therefore, a mapping with RSDFT can be introduced through the introduction of an effective non-divergent interaction representing the usual Coulomb electron-electron interaction projected in an incomplete basis set. First applications to weakly correlated molecular systems have been successfully carried out~\cite{LooPraSceTouGin-JCPL-19}, together with extensions of this approach to the calculations of excitation energies~\cite{GinSceTouLoo-JCP-19} and ionization potentials~\cite{LooPraSceGinTou-ARX-19}. The goal of the present work is to further develop this approach for the description of strongly correlated systems. The paper is organized as follows. In Section \ref{sec:theory} we recall the mathematical framework of the basis-set correction and we present the extension for strongly correlated systems. In particular, we focus on imposition of two important formal properties: size-consistency and spin-multiplet degeneracy. -Then, in Section \ref{sec:results} we apply the method to the calculation of the potential energy curves of the C$_2$, N$_2$, O$_2$, F$_2$, and H$_{10}$ molecules up to the dissociation limit, representing prototypes of strongly correlated systems. Finally, we conclude in Section \ref{sec:conclusion}. - -%%%%%%%%%%%%%%%%%%%%%%%% -\section{Theory} -\label{sec:theory} -%%%%%%%%%%%%%%%%%%%%%%%% -As the theory of the basis-set correction has been exposed in details in Ref. \onlinecite{GinPraFerAssSavTou-JCP-18}, we only briefly recall the main equations and concepts needed for this study in Section \ref{sec:basic}, \ref{sec:wee}, and \ref{sec:mur}. More specifically, in Section \ref{sec:basic} we recall the basic mathematical framework of the present theory by introducing the density functional complementary to a basis set $\Bas$. In Section \ref{sec:wee} we introduce the effective non-divergent interaction in the basis set $\Bas$, which leads us to the definition of the effective local range-separation parameter in Section \ref{sec:mur}. Then, in Section \ref{sec:functional} we expose the new approximate complementary functionals based on RSDFT. The generic form of such functionals is exposed in Section \ref{sec:functional_form}, their properties in the context of the basis-set correction are discussed in Section \ref{sec:functional_prop}, and the specific requirements for strong correlation are discussed in Section \ref{sec:requirements}. Finally, the actual form of the functionals used in this work are introduced in Section \ref{sec:final_def_func}. - -\subsection{Basic formal equations} -\label{sec:basic} - -The exact ground-state energy $E_0$ of a $N$-electron system can in principle be obtained in DFT by a minimization over $N$-electron density $\denr$ -\begin{equation} - \label{eq:levy} - E_0 = \min_{\den} \bigg\{ F[\den] + \int \d \br{} v_{\text{ne}} (\br{}) \denr \bigg\}, -\end{equation} -where $v_{ne}(\br{})$ is the nuclei-electron potential, and $F[\den]$ is the universal Levy-Lieb density functional written with the constrained search formalism as~\cite{Lev-PNAS-79,Lie-IJQC-83} -\begin{equation} - \label{eq:levy_func} - F[\den] = \min_{\Psi \rightarrow \den} \elemm{\Psi}{\kinop +\weeop }{\Psi}, -\end{equation} -where the notation $\Psi \rightarrow \den$ means that the wave function $\Psi$ yields the density $n$. The minimizing density $n_0$ in Eq.~\eqref{eq:levy} is the exact ground-state density. Nevertheless, in practical calculations, the accessible densities are necessarily restricted to the set of densities ``representable in a basis set $\Bas$'', i.e. densities coming from wave functions expandable in the Hilbert space generated by the basis set $\Bas$. In the following, we always implicitly consider only such densities representable in $\Bas$. With this restriction, Eq.~\eqref{eq:levy} gives then an upper bound $E_0^\Bas$ of the exact ground-state energy. Since the density has a fast convergence with the size of the basis set, this restriction is a rather weak one and we can consider that $E_0^\Bas$ is a very good approximation to the exact ground-state energy: $E_0^\Bas \approx E_0$. - -In the present context, it is important to notice that in the definition of Eq.~\eqref{eq:levy_func} the wave functions $\Psi$ involved have no restriction to a finite basis set, i.e. they should be expanded in a complete basis set. In Ref.~\onlinecite{GinPraFerAssSavTou-JCP-18}, it was then propose to decompose $F[\den]$ as -\begin{equation} - \label{eq:def_levy_bas} - F[\den] = \min_{\wf{}{\Bas} \rightarrow \den} \elemm{\wf{}{\Bas}}{\kinop +\weeop}{\wf{}{\Bas}} + \efuncden{\den}, -\end{equation} -where $\wf{}{\Bas}$ are wave functions expandable in the Hilbert space generated by $\basis$, and $\efuncden{\den}$ is the density functional complementary to the basis set $\Bas$ defined as -\begin{equation} - \begin{aligned} - \efuncden{\den} = \min_{\Psi \rightarrow \den} \elemm{\Psi}{\kinop +\weeop }{\Psi}   - - \min_{\Psi^{\Bas} \rightarrow \den} \elemm{\wf{}{\Bas}}{\kinop +\weeop}{\wf{}{\Bas}}. - \end{aligned} -\end{equation} -Introducing the decomposition in Eq. \eqref{eq:def_levy_bas} back into Eq.~\eqref{eq:levy}, we arrive at the following expression for $E_0^\Bas$ -\begin{eqnarray} - \label{eq:E0basminPsiB} - E_0^\Bas &=& \min_{\Psi^{\Bas}} \bigg\{ \elemm{\wf{}{\Bas}}{\kinop +\weeop}{\wf{}{\Bas}} + \efuncden{\den_{{\Psi^{\Bas}}}} -\nonumber\\ -&&\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; + \int \d \br{} v_{\text{ne}} (\br{}) \den_{\Psi^{\Bas}}(\br{}) \bigg\}, -\end{eqnarray} -where the minimization is only over wave functions $\wf{}{\Bas}$ restricted to the basis set $\basis$ and $\den_{{\Psi^{\Bas}}}(\br{})$ refers to the density extracted from $\wf{}{\Bas}$. Therefore, with Eq.~\eqref{eq:E0basminPsiB}, one can properly combine a WFT calculation in a finite basis set with a density functional accounting for the correlation effects not included in the basis set. - -As a simple non-self-consistent version of this approach, we can approximate the minimizing wave function $\Psi^{\Bas}$ in Eq.~\eqref{eq:E0basminPsiB} by the ground-state FCI wave function $\psifci$ within $\Bas$, and we then obtain the following approximation for the exact ground-state energy (see Eqs. (12)-(15) of Ref. \onlinecite{GinPraFerAssSavTou-JCP-18}) -\begin{equation} - \label{eq:e0approx} - E_0 \approx E_0^\Bas \approx \efci + \efuncbasisFCI, -\end{equation} -where $\efci$ and $n_\text{FCI}^\Bas$ are the ground-state FCI energy and density, respectively. As it was originally shown in Ref. \onlinecite{GinPraFerAssSavTou-JCP-18} and further emphasized in Ref. \onlinecite{LooPraSceTouGin-JCPL-19,GinSceTouLoo-JCP-19}, the main role of $\efuncbasisFCI$ is to correct for the basis-set incompleteness error, a large part of which originating from the lack of electron-electron cusp in the wave function expanded in an incomplete basis set. The whole purpose of this work is to determine approximations for $\efuncbasisFCI$ which are suitable for treating strong correlation regimes. Two requirements on the approximations for this purpose are i) size consistency and ii) spin-multiplet degeneracy. - -\subsection{Definition of an effective interaction within $\Bas$} -\label{sec:wee} -As originally shown by Kato\cite{Kat-CPAM-57}, the cusp in the exact wave function originates from the divergence of the Coulomb interaction at the coalescence point. Therefore, a cuspless wave function $\wf{}{\Bas}$ could also be obtained from a Hamiltonian with a non-divergent electron-electron interaction. In other words, the impact of the incompleteness of a finite basis set can be understood as the removal of the divergence of the usual Coulomb electron-electron interaction at the coalescence point. - -As originally derived in Ref. \onlinecite{GinPraFerAssSavTou-JCP-18} (Section D and Appendices), one can obtain an effective non-divergent electron-electron interaction, here referred to as $\wbasis$, which reproduces the expectation value of the Coulomb electron-electron interaction operator over a given wave function $\wf{}{\Bas}$. As we are interested in the behaviour at the coalescence point, we focus on the opposite-spin part of the electron-electron interaction. More specifically, the effective electron-electron interaction associated to a given wave function $\wf{}{\Bas}$ is defined as -\begin{equation} - \label{eq:wbasis} - \wbasis = - \begin{cases} - \fbasis /\twodmrdiagpsi, & \text{if $\twodmrdiagpsi \ne 0$,} -\\ - \infty, & \text{otherwise,} - \end{cases} -\end{equation} -where $\twodmrdiagpsi$ is the opposite-spin pair density associated with $\wf{}{\Bas}$ -\begin{equation} - \twodmrdiagpsi = \sum_{pqrs \in \Bas} \SO{p}{1} \SO{q}{2} \Gam{pq}{rs} \SO{r}{1} \SO{s}{2}, -\end{equation} -and $\Gam{pq}{rs} = 2 \mel*{\wf{}{\Bas}}{ \aic{r_\downarrow}\aic{s_\uparrow}\ai{q_\uparrow}\ai{p_\downarrow}}{\wf{}{\Bas}}$ its associated tensor in a basis of spatial orthonormal orbitals $\{\SO{p}{}\}$, and $\fbasis$ is -\begin{equation} - \label{eq:fbasis} - \fbasis - = \sum_{pqrstu \in \Bas} \SO{p}{1} \SO{q}{2} \V{pq}{rs} \Gam{rs}{tu} \SO{t}{1} \SO{u}{2}, -\end{equation} -with the usual two-electron Coulomb integrals $\V{pq}{rs}=\langle pq | rs \rangle$. -With such a definition, one can show that $\wbasis$ satisfies -\begin{eqnarray} - \frac{1}{2}\iint \dr{1} \dr{2} \wbasis \twodmrdiagpsi = -\nonumber\\ -\frac{1}{2} \iint \dr{1} \dr{2} \frac{\twodmrdiagpsi}{|\br{1}-\br{2}|}. -\end{eqnarray} -As shown in Ref. \onlinecite{GinPraFerAssSavTou-JCP-18}, the effective interaction $\wbasis$ is necessarily finite at coalescence for an incomplete basis set, and tends to the usual Coulomb interaction in the CBS limit for any choice of wave function $\psibasis$, i.e. -\begin{equation} - \label{eq:cbs_wbasis} - \lim_{\Bas \rightarrow \text{CBS}} \wbasis = \frac{1}{|\br{1}-\br{2}|},\quad \forall\,\psibasis. -\end{equation} -The condition in Eq.~\eqref{eq:cbs_wbasis} is fundamental as it guarantees the correct behavior of the theory in the CBS limit. - -\subsection{Definition of a local range-separation parameter} -\label{sec:mur} -\subsubsection{General definition} -As the effective interaction within a basis set, $\wbasis$, is non divergent, it ressembles the long-range interaction used in RSDFT -\begin{equation} - \label{eq:weelr} - w_\text{ee}^{\lr}(\mu;r_{12}) = \frac{\text{erf}\big(\mu \,r_{12} \big)}{r_{12}}, -\end{equation} -where $\mu$ is the range-separation parameter. As originally proposed in Ref. \onlinecite{GinPraFerAssSavTou-JCP-18}, we make the correspondance between these two interactions by using the local range-separation parameter $\murpsi$ -\begin{equation} - \label{eq:def_mur} - \murpsi = \frac{\sqrt{\pi}}{2} \wbasiscoal, -\end{equation} -such that the interactions coincide at the electron-electron colescence point for each $\br{}$ -\begin{equation} - w_\text{ee}^{\lr}(\murpsi;0) = \wbasiscoal, \quad \forall \, \br{}. -\end{equation} -Because of the very definition of $\wbasis$, one has the following property in the CBS limit (see Eq.~\eqref{eq:cbs_wbasis}) -\begin{equation} - \label{eq:cbs_mu} - \lim_{\Bas \rightarrow \text{CBS}} \murpsi = \infty, \quad \forall \,\psibasis, -\end{equation} -which is again fundamental to guarantee the correct behavior of the theory in the CBS limit. - -\subsubsection{Frozen-core approximation} -As all WFT calculations in this work are performed within the frozen-core approximation, we use the valence-only version of the various quantities needed for the complementary basis functional introduced in Ref.~\onlinecite{LooPraSceTouGin-JCPL-19}. We partition the basis set as $\Bas = \Cor \bigcup \BasFC$, where $\Cor$ and $\BasFC$ are the sets of core and active orbitals, respectively, and define the valence-only local range-separation parameter as -\begin{equation} - \label{eq:def_mur_val} - \murpsival = \frac{\sqrt{\pi}}{2} \wbasiscoalval{}, -\end{equation} -where $\wbasisval$ is the valence-only effective interaction defined as -\begin{equation} - \label{eq:wbasis_val} - \wbasisval = - \begin{cases} - \fbasisval /\twodmrdiagpsival, & \text{if $\twodmrdiagpsival \ne 0$,} -\\ - \infty, & \text{otherwise,} - \end{cases} -\end{equation} -where $\fbasisval$ and $\twodmrdiagpsival$ are defined as -\begin{equation} - \label{eq:fbasis_val} - \fbasisval - = \sum_{pq\in \Bas} \sum_{rstu \in \BasFC} \SO{p}{1} \SO{q}{2} \V{pq}{rs} \Gam{rs}{tu} \SO{t}{1} \SO{u}{2}, -\end{equation} -and -\begin{equation} - \label{eq:twordm_val} - \twodmrdiagpsival = \sum_{pqrs \in \BasFC} \SO{p}{1} \SO{q}{2} \Gam{pq}{rs} \SO{r}{1} \SO{s}{2}. -\end{equation} -Notice the restrictions of the sums to the set of active orbitals in Eqs.~\eqref{eq:fbasis_val} and \eqref{eq:twordm_val}. -It is noteworthy that, with the present definition, $\wbasisval$ still tends to the usual Coulomb interaction as $\Bas \to \CBS$. - -\subsection{Generic form and properties of the approximations for $\efuncden{\den}$ } -\label{sec:functional} - -\subsubsection{Generic form of the approximate functionals} -\label{sec:functional_form} - -As originally proposed and motivated in Ref. \onlinecite{GinPraFerAssSavTou-JCP-18}, we approximate the complementary basis functional $\efuncden{\den}$ by using the so-called correlation energy functional with multideterminant reference (ECMD) introduced by Toulouse \textit{et al.}~\cite{TouGorSav-TCA-05}. Following the recent work in Ref.~\onlinecite{LooPraSceTouGin-JCPL-19}, we propose to use a Perdew-Burke-Ernzerhof (PBE)-like functional which uses the total density $\denr$, the spin polarisation $\zeta(\br{})=[n_\uparrow(\br{})-n_\downarrow(\br{})]/\denr$, the reduced density gradient $s(\br{}) = \nabla \denr/\denr^{4/3}$, and the on-top pair density $\ntwo(\br{})\equiv \ntwo(\br{},\br{})$. In the present work, all these quantities are computed with the same wave function $\psibasis$ used to define $\mur \equiv\murpsi$. Therefore, a given approximation X of $\efuncden{\den}$ will have the following generic local form -\begin{equation} - \begin{aligned} - \label{eq:def_ecmdpbebasis} - &\efuncdenpbe{\argebasis} = \;\;\;\;\;\;\;\; \\ &\int \d\br{} \,\denr \ecmd(\argrebasis), - \end{aligned} -\end{equation} -where $\ecmd(\argecmd)$ is the correlation energy per particle taken as -\begin{equation} - \label{eq:def_ecmdpbe} - \ecmd(\argecmd) = \frac{\varepsilon_{\text{c}}^{\text{PBE}}(\argepbe)}{1+ \beta(\argepbe) \; \mu^3}, -\end{equation} -with -\begin{equation} - \label{eq:def_beta} - \beta(\argepbe) = \frac{3}{2\sqrt{\pi}(1 - \sqrt{2})}\frac{\varepsilon_{\text{c}}^{\text{PBE}}(\argepbe)}{\ntwo/\den}, -\end{equation} -where $\varepsilon_{\text{c}}^{\text{PBE}}(\argepbe)$ is the usual PBE correlation energy per particle~\cite{PerBurErn-PRL-96}. Before introducing the different flavors of approximate functionals that we will use here (see Section~\ref{sec:def_func}), we would like to give some motivations for this choice of functional form. - -The functional form of $\ecmd(\argecmd)$ in Eq.~\ref{eq:def_ecmdpbe} has been originally proposed in Ref.~\onlinecite{FerGinTou-JCP-18} in the context of RSDFT. In the $\mu\to 0$ limit, it reduces to the usual PBE correlation functional -\begin{equation} - \lim_{\mu \rightarrow 0} \ecmd(\argecmd) = \varepsilon_{\text{c}}^{\text{PBE}}(\argepbe), -\end{equation} -which is relevant in the weak-correlation (or high-density) limit. In the large-$\mu$ limit, it behaves as -\begin{equation} - \label{eq:lim_mularge} - \ecmd(\argecmd) \isEquivTo{\mu\to\infty} \frac{2\sqrt{\pi}(1 - \sqrt{2})}{3 \mu^3} \frac{\ntwo}{n}, -\end{equation} -which is the exact large-$\mu$ behavior of the exact ECMD correlation energy~\cite{PazMorGorBac-PRB-06,FerGinTou-JCP-18}. Of course, for a specific system, the large-$\mu$ behavior will be exact only if one uses for $n_2$ the \textit{exact} on-top pair density of this system. This large-$\mu$ limit in Eq.~\eqref{eq:lim_mularge} is relevant in the strong-correlation (or low-density) limit. In the context of RSDFT, some of the present authors have illustrated in Ref.~\onlinecite{FerGinTou-JCP-18} that the on-top pair density involved in Eq. \eqref{eq:def_ecmdpbe} plays indeed a crucial role when reaching the strong-correlation regime. The importance of the on-top pair density in the strong-correlation regime have been also recently acknowledged by Gagliardi and coworkers~\cite{CarTruGag-JPCA-17} and Pernal and coworkers\cite{GritMeePer-PRA-18}. - -Note also that $\ecmd(\argecmd)$ vanishes when $\ntwo$ vanishes -\begin{equation} - \label{eq:lim_n2} - \lim_{\ntwo \rightarrow 0} \ecmd(\argecmd) = 0, -\end{equation} -which is expected for systems with a vanishing on-top pair density, such as the totally dissociated H$_2$ molecule which is the archetype of strongly correlated systems. Finally, the function $\ecmd(\argecmd)$ vanishes when $\mu \rightarrow \infty$ like all RSDFT short-range functionals \begin{equation} - \label{eq:lim_muinf} - \lim_{\mu \rightarrow \infty} \ecmd(\argecmd) = 0. -\end{equation} - -\subsubsection{Properties of approximate functionals} -\label{sec:functional_prop} - -Within the definitions of Eqs.~\eqref{eq:def_mur} and \eqref{eq:def_ecmdpbebasis}, any approximate complementary basis functional $\efuncdenpbe{\argebasis}$ satisfies two important properties. - -First, thanks to the properties in Eq.~\eqref{eq:cbs_mu} and~\eqref{eq:lim_muinf}, $\efuncdenpbe{\argebasis}$ vanishes in the CBS limit, whatever the wave function $\psibasis$ used to define the local range-separation parameter $\mu(\br{})$, -\begin{equation} - \label{eq:lim_ebasis} - \lim_{\basis \rightarrow \text{CBS}} \efuncdenpbe{\argebasis} = 0, \quad \forall\, \psibasis, -\end{equation} -which guarantees an unaltered CBS limit. - -Second, the fact that $\efuncdenpbe{\argebasis}$ vanishes for systems with vanishing on-top pair density guarantees the correct limit for one-electron systems and for the stretched H$_2$ molecule. This property is guaranteed independently by i) the definition of the effective interaction $\wbasis$ (see Eq.~\eqref{eq:wbasis}) together with the condition in Eq.~\eqref{eq:lim_muinf}, ii) the fact that $\ecmd(\argecmd)$ vanishes when the on-top pair density vanishes (see Eq.~\eqref{eq:lim_n2}). - -\subsection{Requirements for the approximate functionals in the strong-correlation regime} -\label{sec:requirements} - -\subsubsection{Requirements: size-consistency and spin-multiplet degeneracy} - -An important requirement for any electronic-structure method is size-consistency, i.e. the additivity of the energies of non-interacting fragments, which is mandatory to avoid any ambiguity in computing interaction energies. When two subsystems $A$ and $B$ dissociate in closed-shell systems, as in the case of weak intermolecular interactions for instance, spin-restricted Hartree-Fock (RHF) is size-consistent. When the two subsystems dissociate in open-shell systems, such as in covalent bond breaking, it is well known that the RHF approach fails and an alternative is to use a complete-active-space (CAS) wave function which, provided that the active space has been properly chosen, leads to additive energies. - -Another important requirement is spin-multiplet degeneracy, i.e. the independence of the energy with respect to the $S_z$ component of a given spin state, which is also a property of any exact wave function. Such a property is also important in the context of covalent bond breaking where the ground state of the supersystem $A+B$ is generally low spin while the ground states of the fragments $A$ and $B$ are high spin and can have multiple $S_z$ components. - -\subsubsection{Condition for the functional $\efuncdenpbe{\argebasis}$ to obtain spin-multiplet degeneracy} - -A sufficient condition to achieve spin-multiplet degeneracy is to eliminate all dependencies on $S_z$, which in the case of the functional $\ecmd(\argecmd)$ means removing the dependency on the spin polarization $\zeta(\br{})$ use the PBE correlation functional $\varepsilon_{\text{c}}^{\text{PBE}}(\argepbe)$ (see Eq. \eqref{eq:def_ecmdpbe}). - -It has been proposed to replace in functionals the dependency on the spin polarization by the dependency on the on-top pair density. Most often, it is done by introducing an effective spin polarisation~\cite{MosSan-PRA-91,BecSavSto-TCA-95,Sav-INC-96a,Sav-INC-96,MieStoSav-MP-97,TakYamYam-CPL-02,TakYamYam-IJQC-04,GraCre-MP-05,TsuScuSav-JCP-10,LimCarLuoMaOlsTruGag-JCTC-14,GarBulHenScu-JCP-15,GarBulHenScu-PCCP-15,CarTruGag-JCTC-15,GagTruLiCarHoyBa-ACR-17} (see, also, Refs.~\onlinecite{PerSavBur-PRA-95,StaDav-CPL-01}) -\begin{equation} - \label{eq:def_effspin} - \tilde{\zeta}(n,n_{2}) = -% \begin{cases} - \sqrt{ 1 - 2 \; n_{2}/n^2 }, -% 0 & \text{otherwise.} -% \end{cases} -\end{equation} -expressed as a function of the density $n$ and the on-top pair density $n_2$, calculated from a given wave function. The advantage of this approach is that this effective spin polarisation $\tilde{\zeta}$ is independent from $S_z$, since the on-top pair density is independent from $S_z$. Nevertheless, the use of $\tilde{\zeta}$ in Eq.~\eqref{eq:def_effspin} presents the disadvantage that since this expression was derived for a single-determinant wave function, and it does not appear well justified to use it for a multideterminant wave function as well. In particular, for a multideterminant wave function, it may happen that $1 - 2 \; n_{2}/n^2 < 0 $ and thus in this cas Eq.~\eqref{eq:def_effspin} gives a complex value of $\tilde{\zeta}$~\cite{BecSavSto-TCA-95}. - -%The advantage of this approach are at least two folds: i) the effective spin polarisation $\tilde{\zeta}$ is independent from $S_z$ since the on-top pair density is independent from $S_z$, ii) it introduces an indirect dependency on the on-top pair density of the wave function $\psibasis$ which usually improves the treatment of strong correlation. -%Nevertheless, the use of $\tilde{\zeta}$ presents several disadvantages as it can become complex when $1 - 2 \; n_{2}/n^2 < 0 $ and also -%the formula of equation \eqref{eq:def_effspin} is exact only when the density $n$ and on-top pair density $\ntwo^{\psibasis}$ are obtained from a single determinant\cite{PerSavBur-PRA-95}, but it is applied to multi configurational wave functions. - -An alternative way to eliminate the $S_z$ dependency is to simply set $\zeta=0$, i.e. to always use the spin-unpolarized functional. This lowers the accuracy for open-shell systems at $\mu=0$, i.e. for the usual PBE correlation functional $\varepsilon_{\text{c}}^{\text{PBE}}(\argepbe)$. Nevertheless, we argue that, for $\mu$ sufficiently large, it is a viable option. Indeed, the purpose of introducing the spin polarisation in semilocal density-functional approximations is to mimic the exact on-top pair density~\cite{PerSavBur-PRA-95}, but our functional $\ecmd(\argecmd)$ already explicitly depends on the on-top pair density (see Eq.~\eqref{eq:def_ecmdpbe} and \eqref{eq:def_beta}). The dependencies on $\zeta$ and $n_2$ can thus be expected to be largely redundant. Therefore, we propose here to also test the $\ecmd$ functional with \textit{a zero spin polarisation}. This ensures a $S_z$ independence and, as will be numerically shown, very weakly affects the accuracy of the functional. - - -\subsubsection{Conditions for size consistency} - -Since $\efuncdenpbe{\argebasis}$ is a single integral over $\mathbb{R}^3$ of local quantities ($n(\br{})$, $\zeta(\br{})$, $s(\br{})$, $n_2(\br{})$,$\mu(\br{})$), in the case of non-overlapping fragments $A\ldots B$ it can be written as the sum of two local contributions: one coming from the integration over the region of the subsystem $A$ and the other one from the region of the subsystem $B$. Therefore, a sufficient condition for the size consistency is that these local quantities coincide in the isolated systems and in the subsystems of the supersystem $A\ldots B$. Since these local quantities are calculated from the wave function $\psibasis$, a sufficient condition is that the wave function is multiplicatively separable in the limit of non-interacting fragments, i.e. $\Psi_{A\ldots B}^{\basis} = \Psi_A^{\basis} \Psi_B^{\basis}$. In the case where the two subsystems $A$ and $B$ dissociate in closed-shell systems, a simple RHF wave function ensures this property, but when one or several covalent bonds are broken, the use of a properly chosen CAS wave function is sufficient to recover this property. The condition for the active space involved in the CAS wave function is that it has to lead to size-consistent energies in the limit of dissociated fragments. - - -\subsection{Different types of approximations for the functional} -\label{sec:final_def_func} -\subsubsection{Definition of the protocol to design functionals} - -As the present work focusses on the strong correlation regime, we propose here to investigate only approximate functionals which are $S_z$ independent and size-consistent in the case of covalent bond breaking. Therefore, the wave functions $\psibasis$ used throughout this paper are CAS wave functions in order to ensure size consistency of all local quantities. The difference between the different flavors of functionals are only on i) the type of spin polarisation used, and ii) the type of on-top pair density used. - -Regarding the spin polarisation that enters into $\varepsilon_{\text{c}}^{\text{PBE}}(\argepbe)$, two different types of $S_z$-independent formulations are used: i) the \textit{effective} spin polarization $\tilde{\zeta}$ defined in Eq.~\eqref{eq:def_effspin} and calculated from the CAS wave function, and ii) a \textit{zero} spin polarization. - -Regarding the on-top pair density entering in Eq.~\eqref{eq:def_beta}, we use two different approximations. The first one is based on the uniform-electron gas (UEG) and reads -\begin{equation} - \label{eq:def_n2ueg} - \ntwo^{\text{UEG}}(n,\zeta) \approx n^2\big(1-\zeta^2\big)g_0(n), -\end{equation} -where the pair-distribution function $g_0(n)$ is taken from Eq.~(46) of Ref.~\onlinecite{GorSav-PRA-06}. As the spin polarization appears in Eq.~\eqref{eq:def_n2ueg}, we use the effective spin polarization $\tilde{\zeta}$ of Eq.~\eqref{eq:def_effspin} in order to ensure $S_z$ independence. Thus, $\ntwo^{\text{UEG}}$ will depend indirectly on the on-top pair density of the CAS wave function through $\tilde{\zeta}$. - -Another approach to approximate the exact on top pair density consists in using directly the on-top pair density of the CAS wave function. Following the work of some of the previous authors~\cite{FerGinTou-JCP-18,GinSceTouLoo-JCP-19} we introduce the extrapolated on-top pair density $\ntwoextrap$ as -\begin{equation} - \label{eq:def_n2extrap} - \ntwoextrap(\ntwo,\mu) = \bigg( 1 + \frac{2}{\sqrt{\pi}\mu} \bigg)^{-1} \; \ntwo -\end{equation} -which directly follows from the large-$\mu$ extrapolation of the exact on-top pair density derived by Gori-Giorgi and Savin\cite{GorSav-PRA-06} in the context of RSDFT. When using $\ntwoextrap(\ntwo,\mu)$ in a functional, we will simply refer it as ``ot''. - - -\subsubsection{Definition of functionals with good formal properties} -\label{sec:def_func} - -We define the following functionals:\\ - -i) PBE-UEG-$\tilde{\zeta}$ which uses the UEG on-top pair density defined in Eq.~\eqref{eq:def_n2ueg} and the effective spin polarization of Eq.~\eqref{eq:def_effspin} -\begin{equation} - \label{eq:def_pbeueg} - \begin{aligned} - \bar{E}^\Bas_{\pbeuegXi} = \int \d\br{} \,\denr \ecmd(\argrpbeuegXi), - \end{aligned} -\end{equation} -ii) PBE-ot-$\tilde{\zeta}$ which uses the on-top pair density of Eq.~\eqref{eq:def_n2extrap} -\begin{equation} - \label{eq:def_pbeueg} - \begin{aligned} - \bar{E}^\Bas_{\pbeontXi} = \int \d\br{} \,\denr \ecmd(\argrpbeontXi), - \end{aligned} -\end{equation} -iii) PBE-ot-$0{\zeta}$ where uses zero spin polarization and the on-top pair density of Eq.~\eqref{eq:def_n2extrap} -\begin{equation} - \label{eq:def_pbeueg} - \begin{aligned} - \bar{E}^\Bas_{\pbeontns} = \int \d\br{} \,\denr \ecmd(\argrpbeontns). - \end{aligned} -\end{equation} - -%%%%%%%%%%%%%%%%%%%%%%%% -\section{Results for the C$_2$, N$_2$, O$_2$, F$_2$, and H$_{10}$ potential energy curves} -\label{sec:results} - -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{figure*} - \includegraphics[width=0.45\linewidth]{data/H10/DFT_vdzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/H10/DFT_vdzE_relat_zoom.eps} - \includegraphics[width=0.45\linewidth]{data/H10/DFT_vtzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/H10/DFT_vtzE_relat_zoom.eps} - \includegraphics[width=0.45\linewidth]{data/H10/DFT_vqzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/H10/DFT_vqzE_relat_zoom.eps} - \caption{ - Potential energy curves of the H$_{10}$ chain with equally distant atoms calculated with MRCI+Q and basis-set corrected MRCI+Q using the 1) cc-pVDZ, 2) cc-pVTZ, and 3) cc-pVQZ basis sets. The MRCI+Q energies and the estimated exact energies are from Ref. \onlinecite{h10_prx}. - \label{fig:H10}} -\end{figure*} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% - -\subsection{Computational details} - -The purpose of the present paper being the study of the basis-set correction in the regime of strong correlation, we study the potential energy curves up to the dissociation limit of a H$_{10}$ chain with equally distant atoms and the C$_2$, N$_2$, O$_2$, and F$_2$ molecules. In a given basis set, in order to compute the approximation of the exact ground-state energy using Eq.~\eqref{eq:e0approx}, one needs an approximation to both the FCI energy $\efci$ and the basis-set correction $\efuncbasisFCI$. - -In the case of the C$_2$, N$_2$, O$_2$, and F$_2$ molecules, approximations to the FCI energies are obtained using converged frozen-core (1s orbitals are kept frozen) CIPSI calculations and the extrapolation scheme for the perturbative correction of Umrigar \textit{et. al.} (see Refs. \onlinecite{HolUmrSha-JCP-17, SceGarCafLoo-JCTC-18, LooSceBloGarCafJac-JCTC-18, SceBenJacCafLoo-JCP-18, LooBogSceCafJac-JCTC-19, QP2} for more details) using the Quantum Package software~\cite{QP2}. The estimated exact potential energy curves are obtained from Ref. \onlinecite{LieCle-JCP-74a}. For all geometries and basis sets, the error with respect to the exact FCI energies are estimated to be below 0.5 mH. In the case of the H$_{10}$ chain, the approximation to the FCI energies together with the estimated exact potential energy curves are obtained from the data of Ref. \onlinecite{h10_prx} where the authors performed MRCI+Q calculations with a minimal valence active space as reference (see below for the description of the active space). - -Regarding the complementary basis functional, we first perform full-valence complete-active-space self-consistent-field (CASSCF) calculations with the GAMESS-US software\cite{gamess} to obtain the wave function $\psibasis$. Then, all density-like quantities involved in the functional (density $n(\br{})$, spin polarization $\zeta(\br{})$, reduced density gradient $s(\br{})$, and on-top pair density $n_2(\br{})$) together with the local range-separation function $\mu(\br{})$ of Eq.~\eqref{eq:def_mur} are calculated with this full-valence CASSCF wave function. These CASSCF wave functions correspond to the following active spaces: 10 electrons in 10 orbitals for H$_{10}$, 8 electrons in 8 electrons for C$_2$, 10 electrons in 8 orbitals for N$_2$, 12 electrons in 8 orbitals for O$_2$, and 14 electrons in 8 orbitals for F$_2$. - -Also, as the frozen core approximation is used in all our CIPSI calculations, we use the corresponding valence-only complementary functionals. Therefore, all density-like quantities exclude any contribution from the core 1s orbitals, and the range-separation function is taken as the one defined in Eq.~\eqref{eq:def_mur_val}. - -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{table*} -\label{tab:d0} -\caption{Atomization energies $D_0$ (in mH) and associated errors (in square brackets) with respect to the estimated exact values computed at different approximation levels with different basis sets.} -\begin{ruledtabular} -\begin{tabular}{llcccc} - - System & Basis set & MRCI+Q$^a$ & (MRCI+Q)+$\pbeuegXi$ & (MRCI+Q)+$\pbeontXi$ & (MRCI+Q)+$\pbeontns$ \\ -\hline -H$_{10}$ & cc-pVDZ & 622.1 [43.3] & 642.6 [22.8] & 649.2 [16.2] & 649.5 [15.9] \\ - & cc-pVTZ & 655.2 [10.2] & 661.9 [3.5] & 666.0 [-0.6] & 666.0 [-0.6] \\ - & cc-pVQZ & 661.2 [4.2] & 664.1 [1.3] & 666.4 [-1.0] & 666.5 [-1.1] \\[0.1cm] -%\cline{2-6} - &\multicolumn{5}{c}{Estimated exact$^a$: 665.4} \\[0.2cm] -\hline -System & Basis set & FCI & FCI+$\pbeuegXi$ & FCI+$\pbeontXi$ & FCI+$\pbeontns$\\ -\hline -C$_2$ & aug-cc-pVDZ & 204.6 [29.5] & 218.0 [16.1] & 217.4 [16.7] & 217.0 [17.1] \\ - & aug-cc-pVTZ & 223.4 [10.9] & 228.1 [6.0] & 228.6 [5.5] & 226.5 [5.6] \\[0.1cm] -%\cline{2-6} - & \multicolumn{5}{c}{Estimated exact$^b$: 234.1} \\[0.2cm] -\hline -System & Basis set & FCI & FCI+$\pbeuegXi$ & FCI+$\pbeontXi$ & FCI+$\pbeontns$\\ -\hline -N$_2$ & aug-cc-pVDZ & 321.9 [40.8] & 356.2 [6.5] & 355.5 [7.2] & 354.6 [8.1] \\ - & aug-cc-pVTZ & 348.5 [14.2] & 361.5 [1.2] & 363.5 [-0.5] & 363.2 [-0.3] \\[0.1cm] - & \multicolumn{5}{c}{Estimated exact$^b$: 362.7} \\[0.2cm] -\hline -System & Basis set & FCI & FCI+$\pbeuegXi$ & FCI+$\pbeontXi$ & FCI+$\pbeontns$\\ -\hline -O$_2$ & aug-cc-pVDZ & 171.4 [20.5] & 187.6 [4.3] & 187.6 [4.3] & 187.1 [4.8] \\ - & aug-cc-pVTZ & 184.5 [7.4] & 190.3 [1.6] & 191.2 [0.7] & 191.0 [0.9] \\[0.1cm] - & \multicolumn{5}{c}{Estimated exact$^b$: 191.9} \\[0.2cm] -\hline -System & Basis set & FCI & FCI+$\pbeuegXi$ & FCI+$\pbeontXi$ & FCI+$\pbeontns$\\ -\hline -F$_2$ & aug-cc-pVDZ & 49.6 [12.6] & 54.8 [7.4] & 54.9 [7.3] & 54.8 [7.4] \\ - & aug-cc-pVTZ & 59.3 [2.9] & 61.2 [1.0] & 61.5 [0.7] & 61.5 [0.7] \\[0.1cm] - & \multicolumn{5}{c}{Estimated exact$^b$: 62.2} \\ -\end{tabular} -\end{ruledtabular} -\begin{flushleft} -\vspace{-0.2cm} -$^a$ From Ref. \onlinecite{h10_prx}. \\ -$^b$ From the extrapolated valence-only non-relativistic calculations of Ref. \onlinecite{BytLaiRuedenJCP05}. -\end{flushleft} - -\label{tab:extensiv_closed} -\end{table*} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% - - -\subsection{Dissociation of the H$_{10}$ chain with equally distant atoms} - - -The study of the H$_{10}$ chain with equally distant atoms is a good prototype of strongly-correlated systems as it consists in the simultaneous breaking of 10 covalent $\sigma$ bonds which all interact with each other. Also, being a relatively small system, benchmark calculations at near CBS values can be obtained (see Ref. \onlinecite{h10_prx} for a detailed study of this problem). - -We report in Figure \ref{fig:H10} the potential energy curves computed using the cc-pVXZ (X=D,T,Q) basis sets for different levels of approximations. The computation of the atomization energies $D_0$ at each level of theory used here is reported in Table \ref{tab:d0}. A general trend that can be observed from these data is that, in a given basis set, the quality of the potential energy cruves are globally improved by adding the basis-set correction, whatever the level of approximation used for the functional $\efuncbasisFCI$. Also, no bizarre behaviors are found when stretching the bonds, which shows that the functionals are robust when reaching the strong correlation regime. - -More quantitatively, the values of $D_0$ are within chemical accuracy (i.e., an error below 1.4 mH) from the cc-pVTZ basis set when using the PBE-ot-$\tilde{\zeta}$ and PBE-ot-$0{\zeta}$ functionals, whereas such an accuracy is not reached at the cc-pVQZ basis set using standard MRCI+Q. - -Regarding in more details the performance of the different types of approximate functionals, the results show that PBE-ot-$\tilde{\zeta}$ and PBE-ot-$0{\zeta}$ are very similar (the maximal difference on $D_0$ being 0.3 mH), and they give slightly more accurate results than PBE-UEG-$\tilde{\zeta}$. These findings bring two important clues on the role of the different physical ingredients used in the functionals: i) the explicit use of the on-top pair density coming from the CASSCF wave function (see Eq.~\eqref{eq:def_n2extrap}) is preferable to the use of the on-top pair density based on the UEG (see Eq.~\eqref{eq:def_n2ueg}); ii) removing the dependency on any kind of spin polarization does not lead to significant loss of accuracy provided that one uses a qualitatively correct on-top pair density. Point ii) is important as it shows that spin polarization in density-functional approximations essentially plays the same role as that of the on-top pair density. - -\subsection{Dissociation of the C$_2$, N$_2$, O$_2$, and F$_2$ molecules} - -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{figure*} - \includegraphics[width=0.45\linewidth]{data/C2/DFT_avdzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/C2/DFT_avdzE_relat_zoom.eps} - \includegraphics[width=0.45\linewidth]{data/C2/DFT_avtzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/C2/DFT_avtzE_relat_zoom.eps} - \caption{ - Potential energy curves of the C$_2$ molecule calculated with near-FCI and basis-set corrected near-FCI using the 1) aug-cc-pVDZ and 2) aug-cc-pVTZ basis sets. The estimated exact energies are from Ref. \onlinecite{LieCle-JCP-74a}. - \label{fig:C2}} -\end{figure*} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% - -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{figure*} - \includegraphics[width=0.45\linewidth]{data/N2/DFT_avdzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/N2/DFT_avdzE_relat_zoom.eps} - \includegraphics[width=0.45\linewidth]{data/N2/DFT_avtzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/N2/DFT_avtzE_relat_zoom.eps} - \caption{ - Potential energy curves of the N$_2$ molecule calculated with near-FCI and basis-set corrected near-FCI using the 1) aug-cc-pVDZ and 2) aug-cc-pVTZ basis sets. The estimated exact energies are from Ref. \onlinecite{LieCle-JCP-74a}. - \label{fig:N2}} -\end{figure*} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% - -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{figure*} - \includegraphics[width=0.45\linewidth]{data/O2/DFT_avdzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/O2/DFT_avdzE_relat_zoom.eps} -% \includegraphics[width=0.45\linewidth]{data/O2/DFT_avtzE_relat.eps} -% \includegraphics[width=0.45\linewidth]{data/O2/DFT_avtzE_relat_zoom.eps} - \caption{ - Potential energy curves of the O$_2$ molecule calculated with near-FCI and basis-set corrected near-FCI using the 1) aug-cc-pVDZ and 2) aug-cc-pVTZ basis sets. The estimated exact energies are from Ref. \onlinecite{LieCle-JCP-74a}. - \label{fig:O2}} -\end{figure*} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% - -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{figure*} - \includegraphics[width=0.45\linewidth]{data/F2/DFT_avdzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/F2/DFT_avdzE_relat_zoom.eps} - \includegraphics[width=0.45\linewidth]{data/F2/DFT_avtzE_relat.eps} - \includegraphics[width=0.45\linewidth]{data/F2/DFT_avtzE_relat_zoom.eps} - \caption{ - Potential energy curves of the F$_2$ molecule calculated with near-FCI and basis-set corrected near-FCI using the 1) aug-cc-pVDZ and 2) aug-cc-pVTZ basis sets. The estimated exact energies are from Ref. \onlinecite{LieCle-JCP-74a}. - \label{fig:F2}} -\end{figure*} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% - -The C$_2$, N$_2$, O$_2$ and F$_2$ molecules are complementary to the H$_{10}$ system for the present study as the level of strong correlation increases while stretching the bond similarly to the case of H$_{10}$, but in addition these molecules exhibit more important and versatile types of weak correlations due to the larger number of electrons. Indeed, the short-range correlation effects are known to play a strong differential effect on the computation of $D_0$, while the shape of the curve far from the equilibrium geometry is governed by dispersion interactions which are medium to long-range weak correlation effects. Also, O$_2$ has a triplet ground state and is therefore a good check for the performance of the dependence on the spin polarization of the different types of functionals proposed here. - -We report in Figure \ref{fig:C2}, \ref{fig:N2}, \ref{fig:O2}, and \ref{fig:F2} the potential energy curves computed using the aug-cc-pVDZ and aug-cc-pVTZ basis sets of C$_2$, N$_2$, O$_2$, and N$_2$, respectively, for different approximation levels. The computation of the atomization energies $D_0$ at each level of theory used here is reported in Table \ref{tab:d0}. - -Just as in the case of H$_{10}$, the quality of $D_0$ are globally improved by adding the basis-set correction and it is remarkable that PBE-ot-$\tilde{\zeta}$ and PBE-ot-$0{\zeta}$ give very similar results. The latter observation confirms that the dependency on the on-top pair density allows one to remove the dependency of any kind of spin polarization for a quite wide range of electron density and also for a high-spin system like O$_2$. More quantitatively, an error below 1.0 mH on the estimated exact valence-only $D_0$ is found for N$_2$, O$_2$, and F$_2$ with the aug-cc-pVTZ basis set using the PBE-ot-$0{\zeta}$ functional, whereas such a result is far from reach within the same basis set at the near-FCI level. In the case of C$_2$ with the aug-cc-pVTZ basis set, an error of about 5.5 mH is found with respect to the estimated exact $D_0$. Such an error is remarkably large with respect to the other diatomic molecules studied here and might be associated to the level of strong correlation in the C$_2$ molecule. - -Regarding now the performance of the basis-set correction along the whole potential energy curve, it is interesting to notice that it fails to provide a noticeable improvement far from the equilibrium geometry. Acknowledging that the weak correlation effects in these regions are dominated by dispersion interactions which are long-range effects, the failure of the present approximations for the complementary basis functionals can be understood easily. Indeed, the whole scheme designed here is based on the physics of correlation near the electron-electron cusp: the local range-separation function $\mu(\br{})$ is designed by looking at the electron-electron coalescence point and the ECMD functionals are suited for short-range correlation effects. Therefore, the failure of the present basis-set correction to describe dispersion interactions is expected. - -\section{Conclusion} -\label{sec:conclusion} - -In the present paper we have extended the recently proposed DFT-based basis-set correction to strongly correlated systems. We studied the H$_{10}$, C$_2$, N$_2$, O$_2$, and F$_2$ molecules up to the dissociation limit at near-FCI level in increasing basis sets, and investigated how the basis-set correction affects the convergence toward the CBS limit of the potential energy curves of these molecular systems. - -The DFT-based basis-set correction relies on three aspects: i) the definition of an effective non-divergent electron-electron interaction obtained from the expectation value over a wave function $\psibasis$ of the Coulomb interaction projected into an incomplete basis set $\basis$; ii) the fitting of this effective interaction with the long-range interaction used in RS-DFT, iii) the use of a complementary correlation functional of RS-DFT. In the present paper, we investigated points i) and iii) in the context of strong correlation and focused on potential energy curves and atomization energies. More precisely, we proposed a new scheme to design functionals fulfilling a) spin-multiplet degeneracy, and b) size consistency. To fulfil such requirements we proposed to use CASSCF wave functions leading to size-consistent energies, and to develop functionals using only $S_z$-independent density-like quantities. - -The development of new $S_z$-independent and size-consistent functionals has lead us to investigate the role of two related quantities: the spin-polarization and the on-top pair density. One important result of the present study is that by using functionals \textit{explicitly} depending on the on-top pair density, one can avoid dependence to any form of spin polarization without loss of accuracy. This avoids the commonly used effective spin polarization calculated from a multideterminant wave function originally proposed in Ref. \onlinecite{BecSavSto-TCA-95} which has the disadvantage of possibly become complex-valued for some multideterminant wave functions. From a more fundamental aspect, this shows that the spin polarization in DFT-related frameworks only mimics the role of the on-top pair density. - -Regarding the results of the present approach, the basis-set correction systematically improves the near-FCI calculations in a given basis set. More quantitatively, it is shown that with only triple-zeta quality basis sets chemically accurate atomization energies $D_0$ are obtained for all systems but C$_2$, whereas the uncorrected near-FCI results are far from that accuracy within the same basis set. In the case of C$_2$, an error of 5.5 mH is obtained with respect to the estimated exact $D_0$, and we leave for further study the detailed investigation of the reasons of this relatively unusual poor performance of the basis-set correction. - -Also, it is shown that the basis-set correction gives substantial differential contribution to potential energy curves close to the equilibrium geometries, but at long interatomic distances it cannot recover the dispersion interactions missing because of the incompleteness of the basis set. This behaviour is actually expected as the dispersion interactions are long-range correlation effects and the present approach was designed to only recover electron correlation effects near the electron-electron coalescence. - -Finally, regarding the computational cost of the present approach, it should be stressed (see supplementary information) that it is minor with respect to WFT methods for all systems and basis sets studied here. We thus believe that this approach is a significant step towards calculations near the CBS limit for strongly correlated systems. - -\bibliography{srDFT_SC,biblio} - -\end{document} diff --git a/Revised_Manuscript/srDFT_SCNotes.bib b/Revised_Manuscript/srDFT_SCNotes.bib deleted file mode 100644 index 881f198..0000000 --- a/Revised_Manuscript/srDFT_SCNotes.bib +++ /dev/null @@ -1,2 +0,0 @@ -@CONTROL{REVTEX41Control} -@CONTROL{aip41Control,pages="0",title=""}

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/dev/null @@ -1,3 +0,0 @@ -Redo all the figures with the good nomenclature: -+) show the 0 \xi in the non zoom -+) change the ot for ONT diff --git a/Revised_Manuscript/biblio.bib b/Revised_Manuscript/biblio.bib deleted file mode 100644 index bf6fae9..0000000 --- a/Revised_Manuscript/biblio.bib +++ /dev/null @@ -1,11864 +0,0 @@ -%% This BibTeX bibliography file was created using BibDesk. -%% http://bibdesk.sourceforge.net/ - -%% Created for Pierre-Francois Loos at 2019-12-12 03:48:36 +0100 - - -%% Saved with string encoding Unicode (UTF-8) - - - -@book{AbrSte-BOOK-72, - Address = {New York}, - Author = {M. Abramowitz and I. A. Stegun}, - Publisher = {Dover Publications}, - Title = {Handbook of Mathematical Functions with Formulas, Graphs and Mathematical Tables}, - Year = {1972}} - -@article{AdaBar-CPL-97, - Author = {C. Adamo and V. Barone}, - Journal = {Chem. Phys. Lett.}, - Pages = {242}, - Volume = {274}, - Year = {1997}} - -@article{AdaBar-JCP-98, - Author = {C. Adamo and V. Barone}, - Journal = {J. Chem. Phys.}, - Pages = {664}, - Volume = {108}, - Year = {1998}} - -@article{AdaBar-JCP-99, - Author = {C. Adamo and V. Barone}, - Journal = {J. Chem. Phys.}, - Pages = {6158}, - Volume = {110}, - Year = {1999}} - -@article{AdaDomGil-JCC-99, - Author = {Ross D. Adamson, Jeremy P. Dombroski, Peter M. W. Gill}, - Journal = {J. Comput. Chem.}, - Pages = {921}, - Volume = {{20}}, - Year = {1999}} - -@article{AdaErnScu-JCP-00, - Author = {C. Adamo and M. Ernzerhof and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {2643}, - Volume = {112}, - Year = {2000}} - -@article{AggYanYan-PRA-13, - Author = {{H. van Aggelen, Y. Yang, and W. Yang}}, - Journal = {Phys. Rev. A}, - Pages = {030501(R)}, - Volume = {88}, - Year = {2013}} - -@article{AhnHehVogTraLeuKlo-CP-14, - Author = {S. Ahnen and A.-S. Hehn and K. D. Vogiatzis and M. A. Trachsel and S. Leutwyler and W. Klopper}, - Journal = {Chem. Phys.}, - Pages = {17}, - Volume = {441}, - Year = {2014}} - -@article{AidMogNilJohMikChrSodKon-JCP-08, - Author = {K. Aidas and A. M{\o}gelh{\o}j and E. J. K. Nilsson and M. S. Johnson and K. V. Mikkelsen and O. Christiansen and P. S\"oderhjelm and J. Kongsted}, - Journal = {J. Chem. Phys.}, - Pages = {194503}, - Volume = {128}, - Year = {2008}} - -@article{AkiTen-CPL-08, - Author = {Y. Akinaga and S. Ten-no}, - Journal = {Chem. Phys. Lett.}, - Pages = {348}, - Volume = {462}, - Year = {2008}} - -@article{AkiTen-IJQC-09, - Author = {Y. Akinaga and S. Ten-no}, - Journal = {Int. J. Quantum Chem.}, - Pages = {1905}, - Volume = {109}, - Year = {2009}} - -@article{AlaDeuKneFro-JCP-17, - Author = {M. M. Alam and K. Deur and S. Knecht and E. Fromager}, - Journal = {J. Chem. Phys.}, - Pages = {204105}, - Volume = {147}, - Year = {2017}} - -@article{AlaFro-CPL-12, - Author = {M. M. Alam and E. Fromager}, - Journal = {Chem. Phys. Lett.}, - Pages = {37}, - Volume = {554}, - Year = {2012}} - -@article{AlaKneFro-PRA-16, - Author = {M. Mehboob Alam and S. Knecht and E. Fromager}, - Journal = {Phys. Rev. A}, - Pages = {012511}, - Volume = {94}, - Year = {2016}} - -@article{AleCol-JMS-99, - Author = {S. A. Alexander and R. L. Coldwell}, - Journal = {J. Mol. Struct. (Theochem)}, - Pages = {67}, - Volume = {487}, - Year = {1999}} - -@article{AliDux-MP-90, - Author = {A. Alijah and G. Duxbury}, - Journal = {Mol. Phys.}, - Pages = {605}, - Volume = {70}, - Year = {1990}} - -@article{Ali-JPCA-13, - Author = {Mojtaba Alipour}, - Journal = {J. Phys. Chem. A}, - Pages = {2884}, - Volume = {117}, - Year = {2013}} - -@article{AllKnoTie-PRA-02, - Author = {O. Allard and A. Pashov and H. Kn\"ockel and E. Tiemann}, - Journal = {Phys. Rev. A}, - Pages = {042503}, - Volume = {66}, - Year = {2002}} - -@article{AlmBar-PRB-85, - Author = {C.-O. Almbladh and U. von Barth}, - Journal = {Phys. Rev. B}, - Pages = {3231}, - Volume = {31}, - Year = {1985}} - -@article{AlmKneJenDyaSau-JCP-16, - Author = {{A. Almoukhalalati, S. Knecht, H. J. Aa. Jensen, K. G. Dyall, and T. Saue}}, - Journal = {J. Chem. Phys.}, - Pages = {074104}, - Volume = {145}, - Year = {2016}} - -@article{AlmPed-PRA-84, - Author = {C.-0. Almbladh and A. C. Pedroza}, - Journal = {Phys. Rev. A}, - Pages = {2322}, - Volume = {29}, - Year = {1984}} - -@article{AndGar-JCP-87, - Author = {J. B. Anderson and D. R. Garmer}, - Journal = {J. Chem. Phys.}, - Pages = {1903}, - Title = {{Validity of random walk methods in the limit of small time steps}}, - Volume = {{87}}, - Year = {1987}} - -@article{AndGod-JCP-10, - Author = {{A. G. Anderson and W. A. Goddard III}}, - Journal = {J. Chem. Phys.}, - Pages = {164110}, - Title = {{Generalized valence bond wave functions in quantum Monte Carlo}}, - Volume = {132}, - Year = {2010}} - -@article{AndGod-JCP-10_fr, - Author = {{A. G. Anderson et W. A. Goddard III}}, - Journal = {J. Chem. Phys.}, - Pages = {164110}, - Volume = {132}, - Year = {2010}} - -@article{And-JCP-75, - Author = {J. B. Anderson}, - Journal = {J. Chem. Phys.}, - Pages = {1499}, - Title = {{A random-walk simulation of the Schr\"odinger equation: H$_3^+$}}, - Volume = {63}, - Year = {1975}} - -@article{And-JCP-76, - Author = {J. B. Anderson}, - Journal = {J. Chem. Phys.}, - Pages = {4121}, - Title = {{Quantum chemistry by random walk. H ${^2}P$, H$_3^+$ $D_{3h}$ ${^1}A^{\prime}_1$, H$_2$ ${^3}\Sigma_u^+$, H$_4$ $^1\Sigma_g^+$, Be ${^1}S$}}, - Volume = {65}, - Year = {1976}} - -@article{And-JCP-80, - Author = {J. B. Anderson}, - Journal = {J. Chem. Phys.}, - Pages = {3897}, - Volume = {73}, - Year = {1980}} - -@article{AndLanLun-PRL-96, - Author = {Y. Andersson and D. C. Langreth and B. I. Lundqvist}, - Journal = {Phys. Rev. Lett.}, - Pages = {102}, - Volume = {76}, - Year = {1996}} - -@article{AngBof-IJQC-97, - Author = {J. M. Anglada and J. M. Bofill}, - Journal = {Int. J. Quantum Chem.}, - Pages = {153}, - Volume = {62}, - Year = {1997}} - -@misc{AngGerSavTou-JJJ-XXa, - Author = {J. G. \'Angy\'an and I. Gerber and A. Savin and J. Toulouse}, - Note = {in preparation}, - Volume = {{}}} - -@misc{AngGerSavTou-JJJ-XX, - Author = {J. G. \'Angy\'an and I. Gerber and A. Savin and J. Toulouse}, - Note = {in preparation}, - Volume = {{}}} - -@article{AngGerSavTou-PRA-05, - Author = {J. G. \'Angy\'an and I. C. Gerber and A. Savin and J. Toulouse}, - Journal = {Phys. Rev. A}, - Pages = {012510}, - Title = {van der Waals forces in density functional theory: perturbational long-range electron interaction corrections}, - Volume = {72}, - Year = {2005}} - -@article{Ang-JCP-07, - Author = {J. G. \'Angy\'an}, - Journal = {J. Chem. Phys.}, - Pages = {024108}, - Title = {On the exchange-hole model of London dispersion forces}, - Volume = {127}, - Year = {2007}} - -@article{AngLiuTouJan-JCTC-11, - Author = {J. G. \'Angy\'an and R.-F. Liu and J. Toulouse and G. Jansen}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3116}, - Title = {Correlation Energy Expressions from the Adiabatic-Connection Fluctuation-Dissipation Theorem Approach}, - Volume = {7}, - Year = {2011}} - -@misc{AngLiuTouJan-JJJ-XX, - Author = {J. G. \'Angyan and R.-F. Liu and J. Toulouse and G. Jansen}, - Note = {J. Chem. Theory Comput., in press.}} - -@article{Ang-PRA-08, - Author = {J. G. \'Angy\'an}, - Journal = {Phys. Rev. A}, - Pages = {022510}, - Volume = {78}, - Year = {2008}} - -@article{AquBarRoo-JCP-03, - Author = {F. Aquilante and V. Barone and B. O. Roos}, - Journal = {J. Chem. Phys.}, - Pages = {12323}, - Volume = {119}, - Year = {2003}} - -@article{ArbKau-CPL-03, - Author = {A. V. Arbuznikov and M. Kaupp}, - Journal = {Chem. Phys. Lett.}, - Pages = {495}, - Volume = {381}, - Year = {2003}} - -@article{ArbKauMalRevMal-PCCP-02, - Author = {A. V. Arbuznikov and M. Kaupp and V. G. Malkin and R. Reviakine and O. L. Malkina}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {5467}, - Volume = {4}, - Year = {2002}} - -@article{Arg-PR-67, - Author = {P. N. Argyres}, - Journal = {Phys. Rev.}, - Pages = {410}, - Volume = {{154}}, - Year = {1967}} - -@article{AriPorBueGal-JPB-95, - Author = {F. Arias de Saavedra and I. Porras and E. Buend\'ia and F. J. G\'alvez}, - Journal = {J. Phys. B}, - Pages = {3123}, - Volume = {28}, - Year = {1995}} - -@article{ArmMat-PRB-02, - Author = {R. Armiento and A. E. Mattsson}, - Journal = {Phys. Rev. B}, - Keywords = {density functional theory; exchange interactions (electron); electron correlations; harmonic oscillators; electron gas}, - Number = {16}, - Pages = {165117}, - Publisher = {APS}, - Title = {Subsystem functionals in density-functional theory: Investigating the exchange energy per particle}, - Volume = {66}, - Year = {2002}} - -@article{ArmMat-PRB-03, - Author = {R. Armiento and A. E. Mattsson}, - Journal = {Phys. Rev. B}, - Keywords = {density functional theory; exchange interactions (electron); electron correlations}, - Number = {24}, - Pages = {245120}, - Publisher = {APS}, - Title = {Alternative separation of exchange and correlation in density-functional theory}, - Volume = {68}, - Year = {2003}} - -@article{ArtMil-PRA-91, - Author = {E. Artacho and L. Mil\'ans~del~Bosch}, - Journal = {Phys. Rev. A}, - Pages = {5770}, - Volume = {{43}}, - Year = {1991}} - -@article{AryGunRub-EPL-02, - Author = {F. Aryasetiawan and O. Gunnarsson and A. Rubio}, - Journal = {Europhys. Lett.}, - Pages = {683}, - Volume = {57}, - Year = {2002}} - -@misc{Ary-JJJ-XX, - Author = {Ferdi Aryasetiawan}, - Note = {http://www.teorfys.lu.se/staff/Claudio.Verdozzi/FunctionalD.pdf}} - -@article{AryMiyTer-PRL-02, - Author = {Aryasetiawan, F. and Miyake, T. and Terakura, K.}, - Journal = {Phys. Rev. Lett.}, - Pages = {166401}, - Title = {Total Energy Method from Many-Body Formulation}, - Volume = {88}, - Year = {2002}} - -@article{AspElaGroLes-JCP-04, - Author = {A. Aspuru-Guzik and O. El Akramine and J. C. Grossman and W. A. Lester}, - Journal = {J. Chem. Phys.}, - Pages = {3049}, - Volume = {120}, - Year = {2004}} - -@article{AssCaf-JCP-00, - Author = {R. Assaraf and M. Caffarel}, - Journal = {J. Chem. Phys.}, - Pages = {4028}, - Title = {{Computing forces with quantum Monte Carlo}}, - Volume = {113}, - Year = {2000}} - -@article{AssCaf-JCP-03, - Author = {R. Assaraf and M. Caffarel}, - Journal = {J. Chem. Phys.}, - Pages = {10536}, - Title = {{Zero-variance zero-bias principle for observables in quantum Monte Carlo: Application to forces}}, - Volume = {119}, - Year = {2003}} - -@article{AssCafKhe-PRE-00, - Author = {R. Assaraf and M. Caffarel and A. Khelif}, - Journal = {Phys. Rev. E}, - Pages = {4566}, - Title = {{Diffusion Monte Carlo methods with a fixed number of walkers}}, - Volume = {61}, - Year = {2000}} - -@article{AssCafKol-PRL-11, - Author = {R. Assaraf and M. Caffarel and A. C. Kollias}, - Journal = {Phys. Rev. Lett.}, - Pages = {150601}, - Title = {Chaotic versus Nonchaotic Stochastic Dynamics in Monte Carlo Simulations: A Route for Accurate Energy Differences in N-Body Systems}, - Volume = {106}, - Year = {2011}} - -@article{AssCaf-PRL-99, - Author = {R. Assaraf and M. Caffarel}, - Journal = {Phys. Rev. Lett.}, - Pages = {4682}, - Title = {{Zero-variance principle for Monte Carlo algorithms}}, - Volume = {83}, - Year = {1999}} - -@article{AssCafSce-PRE-07, - Author = {R. Assaraf and M. Caffarel and A. Scemama}, - Journal = {Phys. Rev. E}, - Pages = {035701(R)}, - Title = {{Improved Monte Carlo estimators for the one-body density}}, - Volume = {75}, - Year = {2007}} - -@article{AssMorFil-JCTC-17, - Author = {R. Assaraf and S. Moroni and C. Filippi}, - Journal = {J. Chem. Theory Comput.}, - Pages = {5273}, - Title = {Optimizing the Energy with Quantum Monte Carlo: A Lower Numerical Scaling for Jastrow-Slater Expansions}, - Volume = {13}, - Year = {2017}} - -@article{atchity:3790, - Author = {Gregory J. Atchity and Klaus Ruedenberg}, - Journal = {The Journal of Chemical Physics}, - Keywords = {ELECTRON CORRELATION; DIABATIC APPROXIMATION; ADIABATIC APPROXIMATION; MATRICES; ELECTRONIC STRUCTURE; POTENTIAL ENERGY; ENERGY LEVELS; IRREDUCIBLE REPRESENTATIONS; SPECTRAL SHIFT; LEVEL CROSSING; QUANTUM CHEMISTRY}, - Number = {5}, - Pages = {3790-3798}, - Publisher = {AIP}, - Title = {Strong shifts in diabatic nondynamic electron correlations cause conical intersection between low-lying closed-shell adiabatic singlets of like symmetry in ozone}, - Url = {http://link.aip.org/link/?JCP/99/3790/1}, - Volume = {99}, - Year = {1993}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/99/3790/1}} - -@article{AusZubLes-CR-12, - Author = {B. M. Austin and D. Yu. Zubarev and W. A. Lester}, - Journal = {Chem. Rev.}, - Pages = {263}, - Title = {{Quantum Monte Carlo and related approaches}}, - Volume = {112}, - Year = {2012}} - -@article{AvePai-PRB-81, - Author = {F. W. Averill and G. S. Painter}, - Journal = {Phys. Rev. B}, - Pages = {6795}, - Volume = {24}, - Year = {1981}} - -@article{AvePai-PRB-92, - Author = {F. W. Averill and G. S. Painter}, - Journal = {Phys. Rev. B}, - Pages = {2498}, - Volume = {46}, - Year = {1992}} - -@article{AyeLevNag-PRA-12, - Author = {P. W. Ayers and M. Levy and A. Nagy}, - Journal = {Phys. Rev. A}, - Pages = {042518}, - Volume = {85}, - Year = {2012}} - -@article{AyeLev-PRA-09, - Author = {P. W. Ayers and M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {012508}, - Volume = {80}, - Year = {2009}} - -@article{AziSla-CP-89, - Author = {R. A. Aziz and M. J. Slaman}, - Journal = {Chem. Phys.}, - Pages = {187}, - Volume = {130}, - Year = {1989}} - -@article{BadHayNee-PRB-08, - Author = {A. Badinski and P. D. Haynes and R. J. Needs}, - Journal = {Phys. Rev. B}, - Pages = {085111}, - Title = {{Nodal Pulay terms for accurate diffusion quantum Monte Carlo forces}}, - Volume = {77}, - Year = {2008}} - -@article{BadHayTraNee-JPCM-10, - Author = {A. Badinski and P. D. Haynes and J. R. Trail and R. J. Needs}, - Journal = {J. Phys.: Condens. Matter}, - Pages = {074202}, - Volume = {22}, - Year = {2010}} - -@article{BaeGri-JPCA-97, - Author = {E. J. Baerends and O. V. Gritsenko}, - Journal = {J. Phys. Chem. A}, - Pages = {5383}, - Volume = {101}, - Year = {1997}} - -@article{BaeLivSal-ARPC-10, - Author = {R. Baer and E. Livshits and U. Salzner}, - Journal = {Annu. Rev. Phys. Chem.}, - Pages = {85}, - Volume = {61}, - Year = {2010}} - -@misc{BaeNeu-JJJ-XX, - Author = {Roi Baer and Daniel Neuhauser}, - Note = {unpublished}} - -@article{BaeNeu-PRL-05, - Author = {Roi Baer and Daniel Neuhauser}, - Journal = {Phys. Rev. Lett.}, - Number = {4}, - Pages = {043002}, - Title = {Density Functional Theory with Correct Long-Range Asymptotic Behavior}, - Volume = {94}, - Year = {2005}} - -@article{Bae-PRL-01, - Author = {E. J. Baerends}, - Journal = {Phys. Rev. Lett.}, - Pages = {133004}, - Volume = {87}, - Year = {2001}} - -@article{BagMad-JPB-11, - Author = {J. C. Baggesen and L. B. Madsen}, - Journal = {J. Phys. B}, - Pages = {115601}, - Volume = {44}, - Year = {2011}} - -@article{BajMitDroWag-PRL-06, - Author = {M. Bajdich and L. Mitas and G. Drobn\'y and L. K. Wagner}, - Journal = {Phys. Rev. Lett.}, - Pages = {130201}, - Volume = {96}, - Year = {2006}} - -@article{BajMitWagSch-PRB-08, - Author = {M. Bajdich and L. Mitas and L. K. Wagner and K. E. Schmidt}, - Journal = {Phys. Rev. B}, - Pages = {115112}, - Title = {Pfaffian pairing and backflow wavefunctions for electronic structure quantum Monte Carlo methods}, - Volume = {77}, - Year = {2008}} - -@article{BajTiaHooKenReb-PRL-10, - Author = {M. Bajdich and M. L. Tiago and R. Q. Hood and P. R. C. Kent and F. A. Reboredo}, - Journal = {Phys. Rev. Lett.}, - Pages = {193001}, - Title = {{Systematic Reduction of Sign Errors in Many-Body Calculations of Atoms and Molecules}}, - Volume = {104}, - Year = {2010}} - -@article{BakFreHilMor-PRA-90, - Author = {{J. D. Baker, D. E. Freund, R. N. Hill, and J. D. Morgan III}}, - Journal = {Phys. Rev. A}, - Pages = {1247}, - Volume = {41}, - Year = {1990}} - -@article{Bak-JCC-86, - Author = {J. Baker}, - Journal = {J. Comput. Chem.}, - Pages = {385}, - Volume = {7}, - Year = {1986}} - -@article{BalDou-CJP-70, - Author = {W. J. Balfour and A. E. Douglas}, - Journal = {Can. J. Phys.}, - Pages = {901}, - Volume = {48}, - Year = {1970}} - -@article{BanAdaSimShe-JPC-85, - Author = {A. Banerjee and N. Adams and J. Simons and R. Shepard}, - Journal = {J. Phys. Chem.}, - Pages = {52}, - Volume = {89}, - Year = {1985}} - -@article{BanAutCha-PRA-08, - Author = {A. Banerjee and J. Autschbach and A. Chakrabarti}, - Journal = {Phys. Rev. A}, - Pages = {032704}, - Volume = {78}, - Year = {2008}} - -@article{BanChaGha-JCP-07, - Author = {A. Banerjee and A. Chakrabarti and T. K. Ghanty}, - Journal = {J. Chem. Phys.}, - Pages = {134103}, - Volume = {127}, - Year = {2007}} - -@article{BanGre-IJQC-76, - Author = {A. Banerjee and F. Grein}, - Journal = {Int. J. Quantum Chem.}, - Pages = {123}, - Volume = {10}, - Year = {1976}} - -@article{BanHar-JCP-02, - Author = {A. Banerjee and M. K. Harbola}, - Journal = {J. Chem. Phys.}, - Pages = {7845}, - Volume = {117}, - Year = {2002}} - -@article{BarAda-CPL-94, - Author = {V. Barone and C. Adamo}, - Journal = {Chem. Phys. Lett.}, - Pages = {432}, - Title = {Theoretical study of direct and water-assisted isomerization of formaldehyde radical cation. A comparison between density functional and post-Hartree-Fock approaches}, - Volume = {224}, - Year = {1994}} - -@article{BarGraHirIva-JCP-05, - Author = {R. J. Bartlett and I. Grabowski and S. Hirata and S. Ivanov}, - Journal = {J. Chem. Phys.}, - Pages = {034104}, - Volume = {122}, - Year = {2005}} - -@article{BarHed-JPC-72, - Author = {U. von Barth and L. Hedin}, - Journal = {J. Phys. C}, - Pages = {1629}, - Volume = {5}, - Year = {1972}} - -@article{BarHol-PRB-96, - Author = {U. von Barth and B. Holm}, - Journal = {Phys. Rev. B}, - Pages = {8411}, - Volume = {{54}}, - Year = {1996}} - -@article{Bar-MP-10, - Author = {R. J. Bartlett}, - Journal = {Mol. Phys.}, - Pages = {3299}, - Volume = {108}, - Year = {2010}} - -@article{BarMus-RMP-07, - Author = {R. J. Bartlett and M. Musia\l}, - Journal = {Rev. Mod. Phys.}, - Pages = {291}, - Title = {Coupled-cluster theory in quantum chemistry}, - Volume = {79}, - Year = {2007}} - -@article{BarPar-JCP-80, - Author = {Libero J. Bartolotti and Robert G. Parr}, - Journal = {The Journal of Chemical Physics}, - Keywords = {FUNCTIONALS; THOMAS-FERMI MODEL; THERMODYNAMIC MOLECULAR MODEL; ENERGY; CORRELATION FUNCTIONS}, - Number = {3}, - Pages = {1593-1596}, - Publisher = {AIP}, - Title = {The concept of pressure in density functional theory}, - Url = {http://link.aip.org/link/?JCP/72/1593/1}, - Volume = {72}, - Year = {1980}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/72/1593/1}} - -@article{BarSorGui-JCTC-12, - Author = {M. Barborini and S. Sorella and L. Guidoni}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1260}, - Title = {Structural Optimization by Quantum Monte Carlo: Investigating the Low-Lying Excited States of Ethylene}, - Volume = {8}, - Year = {2012}} - -@article{Bar-WIRES-12, - Author = {R. J. Bartlett}, - Journal = {WIREs Comput. Mol. Sci.}, - Note = {doi: 10.1002/wcms.76}, - Pages = {126}, - Title = {Coupled-cluster theory and its equation-of-motion extensions}, - Volume = {2}, - Year = {2012}} - -@article{BasJenSau-IJQC-09, - Author = {R. Bast and H. J. Aa. Jensen and T. Saue}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {2091}, - Volume = {109}, - Year = {2009}} - -@article{Bas-PRB-85, - Author = {Ronald Bass}, - Journal = {Phys. Rev. B}, - Pages = {2670}, - Volume = {32}, - Year = {1985}} - -@article{BauAhl-CPL-96, - Author = {R. Bauernschmitt and R. Ahlrichs}, - Journal = {Chem. Phys. Lett.}, - Pages = {454}, - Volume = {256}, - Year = {1996}} - -@article{BauAndRoh-JCTC-12, - Author = {B. Baumeier and D. Andrienko and M. Rohlfing}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2790}, - Volume = {8}, - Year = {2012}} - -@article{BayKad-PR-61, - Author = {G. Baym and L. P. Kadanoff}, - Journal = {Phys. Rev.}, - Pages = {287}, - Volume = {{124}}, - Year = {1961}} - -@article{Bay-PR-62, - Author = {G. Baym}, - Journal = {Phys. Rev.}, - Pages = {1391}, - Volume = {{127}}, - Year = {1962}} - -@article{Bec-IJQC-83, - Author = {A. D. Becke}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {1915}, - Volume = {{23}}, - Year = {1983}} - -@article{BecInuKin-JCP-70, - Author = {R. S. Becker and K. Inuzuka and J. King}, - Journal = {J. Chem. Phys.}, - Pages = {5164}, - Volume = {52}, - Year = {1970}} - -@article{Bec-JCP-03, - Author = {A. D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {2972}, - Volume = {119}, - Year = {2003}} - -@article{Bec-JCP-14, - Author = {A. D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {18A301}, - Volume = {140}, - Year = {2014}} - -@article{Bec-JCP-86, - Author = {A. D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {4524}, - Volume = {{84}}, - Year = {1986}} - -@article{Bec-JCP-88b, - Author = {A. D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {2547}, - Volume = {{88}}, - Year = {1988}} - -@article{Bec-JCP-92a, - Author = {Axel D. Becke}, - Issue = {3}, - Journal = {The Journal of Chemical Physics}, - Keywords = {DENSITY FUNCTIONAL METHOD; THERMOCHEMICAL PROCESSES; DIATOMIC MOLECULES; POLYATOMIC MOLECULES; EXCHANGE INTERACTIONS; CORRECTIONS; ATOMIZATION; GAUSS FUNCTION; N CODES; NUMERICAL SOLUTION; MOLECULES; ERRORS}, - Page = {2155-2160}, - Publisher = {AIP}, - Title = {Density-functional thermochemistry. I. The effect of the exchange-only gradient correction}, - Url = {http://link.aip.org/link/?JCP/96/2155/1}, - Volume = {96}, - Year = {1992}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/96/2155/1}} - -@article{Bec-JCP-92b, - Author = {Axel D. Becke}, - Issue = {12}, - Journal = {The Journal of Chemical Physics}, - Keywords = {DENSITY FUNCTIONAL METHOD; EXCHANGE INTERACTIONS; CORRELATION FUNCTIONS; SPIN DENSITY; CORRECTIONS; SURVEYS; IONIZATION POTENTIAL; ATOMS; MOLECULES; AFFINITY; PROTONS; ATOMIZATION; THERMOCHEMICAL PROCESSES; DATA BASE MANAGEMENT}, - Page = {9173-9177}, - Publisher = {AIP}, - Title = {Density-functional thermochemistry. II. The effect of the Perdew--Wang generalized-gradient correlation correction}, - Url = {http://link.aip.org/link/?JCP/97/9173/1}, - Volume = {97}, - Year = {1992}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/97/9173/1}} - -@article{Bec-JCP-93a, - Author = {Axel D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {1372}, - Title = {A new mixing of Hartree--Fock and local density-functional theories}, - Volume = {98}, - Year = {1993}} - -@article{Bec-JCP-93, - Author = {Axel D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {5648}, - Title = {Density-functional thermochemistry. III. The role of exact exchange}, - Volume = {98}, - Year = {1993}} - -@article{Bec-JCP-96, - Author = {Axel D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {1040}, - Title = {Density-functional thermochemistry. IV. A new dynamical correlation functional and implications for exact-exchange mixing}, - Volume = {104}, - Year = {1996}} - -@article{Bec-JCP-97, - Author = {Axel D. Becke}, - Journal = {J. Chem. Phys.}, - Number = {20}, - Pages = {8554}, - Volume = {107}, - Year = {1997}} - -@article{Bec-JCP-98, - Author = {Axel D. Becke}, - Journal = {J. Chem. Phys.}, - Number = {6}, - Pages = {2092}, - Volume = {109}, - Year = {1998}} - -@article{BecJoh-JCP-05, - Author = {A. D. Becke and E. R. Johnson}, - Journal = {J. Chem. Phys.}, - Pages = {154104}, - Volume = {122}, - Year = {2005}} - -@article{BecJoh-JCP-07, - Author = {A. D. Becke and E. R. Johnson}, - Journal = {J. Chem. Phys.}, - Pages = {154108}, - Volume = {127}, - Year = {2007}} - -@article{Bec-PRA-88, - Author = {A. D. Becke}, - Journal = {Phys. Rev. A}, - Pages = {3098}, - Volume = {{38}}, - Year = {1988}} - -@article{BecSavSto-TCA-95, - Author = {A. D. Becke and A. Savin and H. Stoll}, - Journal = {Theoret. Chim. Acta}, - Pages = {147}, - Volume = {{91}}, - Year = {1995}} - -@article{BecStaBurBla-CP-08, - Author = {E. V. Beck and E. A. Stahlberg and L. W. Burggraf and J.-P. Blaudeau}, - Journal = {Chem. Phys.}, - Pages = {158}, - Volume = {349}, - Year = {2008}} - -@article{BenDisLocChaHea-JPCA-08, - Author = {{T. Benighaus, R. A. DiStasio Jr., R. C. Lochan, J.-D. Chai and M. Head-Gordon}}, - Journal = {J. Phys. Chem. A}, - Pages = {2702}, - Volume = {112}, - Year = {2008}} - -@article{BenMay-CPL-98, - Author = {N. Ben Amor and D. Maynau}, - Journal = {Chem. Phys. Lett.}, - Pages = {211}, - Volume = {{286}}, - Year = {1998}} - -@book{BenOrs-BOOK-99, - Address = {New York}, - Author = {C. M. Bender and S. A. Orszag}, - Publisher = {Springer}, - Title = {Advanced Mathematical Methods for Scientists and Engineers I: Asymptotic Methods and Perturbation Theory}, - Year = {1999}} - -@article{BenPal-JCP-80, - Author = {M. B\'enard and J. Paldus}, - Journal = {J. Chem. Phys.}, - Pages = {6546}, - Volume = {72}, - Year = {1980}} - -@article{BerGriHie-PRA-06, - Author = {R. A. Bertlmann and W. Grimus and B. C. Hiesmayr}, - Journal = {Phys. Rev. A}, - Pages = {054101}, - Volume = {73}, - Year = {2006}} - -@article{BerLinOlsFul-MP-99, - Author = {A. Bernhardsson and R. Lindh and J. Olsen and M. F\"ulscher}, - Journal = {Mol. Phys.}, - Pages = {617}, - Volume = {{96}}, - Year = {1999}} - -@article{BerShaKry-JCP-12, - Author = {Y. A. Bernard and Y. Shao and A. I. Krylov}, - Journal = {J. Chem. Phys.}, - Pages = {204103}, - Title = {General formulation of spin-flip time-dependent density functional theory using non-collinear kernels: Theory, implementation, and benchmarks}, - Volume = {136}, - Year = {2012}} - -@article{Bes-JCP-06, - Author = {Nicholas A. Besley}, - Journal = {J. Chem. Phys.}, - Pages = {074104}, - Volume = {125}, - Year = {2006}} - -@book{BetSal-BOOK-57, - Address = {Berlin}, - Author = {H. A. Bethe and E. E. Salpeter}, - Publisher = {Springer}, - Title = {Quantum Mechanics of one- and two-electron atoms}, - Year = {1957}} - -@article{BisLuh-PRB-82, - Author = {R. F. Bishop and K. H. L\"{u}hrmann}, - Journal = {Phys. Rev. B}, - Pages = {5523}, - Volume = {{26}}, - Year = {1982}} - -@article{Bis-TCA-91, - Author = {R.F. Bishop}, - Journal = {Theoret. Chim. Acta}, - Pages = {95}, - Volume = {{80}}, - Year = {1991}} - -@article{BlaAtt-APL-11, - Author = {X. Blase and C. Attaccalite}, - Journal = {Appl. Phys. Lett.}, - Pages = {171909}, - Volume = {99}, - Year = {2011}} - -@article{BlaYouRoo-JACS-37, - Author = {F. E. Blacet and W. G. Young and J. G. Roof}, - Journal = {J. Am. Chem. Soc.}, - Pages = {608}, - Volume = {59}, - Year = {1937}} - -@article{BleHesGor-JCP-13, - Author = {P. Bleiziffer and A. He{\ss}elmann and A. G\"orling}, - Journal = {J. Chem. Phys.}, - Pages = {084113}, - Volume = {139}, - Year = {2013}} - -@article{BloGraBau-JACS-84, - Author = {C. E. Blom and G. Grassi and A. Bauder}, - Journal = {J. Am. Chem. Soc.}, - Pages = {7427}, - Volume = {106}, - Year = {1984}} - -@incollection{BobGod-INC-77, - Address = {New York}, - Author = {{F. W. Bobrowicz and W. A. Goddard III}}, - Booktitle = {Methods of Electronic Structure Theory, Modern Theoretical Chemistry}, - Editor = {{H. F. Schaeffer III}}, - Pages = {79}, - Publisher = {Plenum}, - Volume = {3}, - Year = {1977}} - -@article{BoeHan-JCP-02, - Author = {A. Daniel Boese and Nicholas C. Handy}, - Journal = {J. Chem. Phys.}, - Number = {22}, - Pages = {9559}, - Volume = {116}, - Year = {2002}} - -@article{BoeMar-JCP-04, - Author = {A. Daniel Boese and Jan M. L. Martin}, - Journal = {J. Chem. Phys.}, - Number = {8}, - Pages = {3405}, - Volume = {121}, - Year = {2004}} - -@article{BohPin-PR-51, - Author = {D. Bohm and D. Pines}, - Journal = {Phys. Rev.}, - Pages = {625}, - Volume = {82}, - Year = {1951}} - -@article{BohPin-PR-53, - Author = {D. Bohm and D. Pines}, - Journal = {Phys. Rev.}, - Pages = {609}, - Title = {A Collective Description of Electron Interactions: III. Coulomb Interactions in a Degenerate Electron Gas}, - Volume = {{92}}, - Year = {1953}} - -@article{Bon-CPL-84, - Author = {V. E. Bondybey}, - Journal = {Chem. Phys. Lett.}, - Pages = {436}, - Volume = {109}, - Year = {1984}} - -@article{BonEng-JCP-84, - Author = {V. E. Bondybey and J. H. English}, - Journal = {J. Chem. Phys.}, - Pages = {568}, - Volume = {80}, - Year = {1984}} - -@article{BooCleThoAla-JCP-11, - Author = {G. H. Booth and D. Cleland and A. J. W. Thom and A. Alavi}, - Journal = {J. Chem. Phys.}, - Pages = {084104}, - Volume = {135}, - Year = {2011}} - -@article{BooGruKreAla-Nat-13, - Author = {G. H. Booth and A. Gr\"uneis and G. Kresse and A. Alavi}, - Journal = {Nature}, - Pages = {365}, - Title = {Towards an exact description of electronic wavefunctions in real solids}, - Volume = {493}, - Year = {2013}} - -@article{BooThoAla-JCP-09, - Author = {G. H. Booth and A. J. W. Thom and A. Alavi}, - Journal = {J. Chem. Phys.}, - Number = {{5}}, - Title = {{Fermion Monte Carlo without fixed nodes: A game of life, death, and annihilation in Slater determinant space}}, - Volume = {{131}}, - Year = {{2009}}} - -@article{BorJorNicNac-TCA-98, - Author = {P. Borowski and K. D. Jordan and J. Nichols and P. Nachtigall}, - Journal = {Theor. Chem. Acc.}, - Pages = {135}, - Volume = {99}, - Year = {1998}} - -@article{BouBenMayCaf-JCP-09, - Author = {T. Bouab\c{c}a and N. Ben Amor and D. Maynau and M. Caffarel}, - Journal = {J. Chem. Phys.}, - Pages = {114107}, - Volume = {130}, - Year = {2009}} - -@article{BouBraCaf-JCP-10, - Author = {T. Bouab\c{c}a and B. Bra\"ida and M. Caffarel}, - Journal = {J. Chem. Phys.}, - Pages = {044111}, - Title = {Multi-Jastrow trial wavefunctions for electronic structure calculations with quantum Monte Carlo}, - Volume = {133}, - Year = {2010}} - -@article{BouChiLegDucBlaJac-JCTC-14, - Author = {{P. Boulanger, S. Chibani, B. Le Guennic, I. Duchemin, X. Blase, and D. Jacquemin}}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4548}, - Volume = {10}, - Year = {2014}} - -@article{BouJacDucBla-JCTC-14, - Author = {P. Boulanger and D. Jacquemin and I. Duchemin and X. Blase}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1212}, - Volume = {10}, - Year = {2014}} - -@article{BowSugAld-PRB-94, - Author = {C. Bowen and G. Sugiyama and B. J. Alder}, - Journal = {Phys. Rev. B}, - Pages = {14838}, - Volume = {{50}}, - Year = {1996}} - -@article{BoyCou-JPB-73, - Author = {R. J. Boyd and C. A. Coulson}, - Journal = {J. Phys. B}, - Pages = {782}, - Volume = {6}, - Year = {1973}} - -@article{BoySarUga-JPB-88, - Author = {R. J. Boyd and C. Sarasola and J. M. Ugalde}, - Journal = {J. Phys. B}, - Pages = {2555}, - Volume = {21}, - Year = {1988}} - -@article{BraHib-02, - Author = {B. Braida and L. Thogersen and W. Wu and P. C. Hiberty}, - Journal = {J. Am. Chem. Soc.}, - Pages = {11781}, - Volume = {124}, - Year = {2002}} - -@article{BraHib-04, - Author = {B. Braida and P. C. Hiberty}, - Journal = {J. Am. Chem. Soc.}, - Pages = {14890}, - Volume = {126}, - Year = {2004}} - -@article{BraHib-08, - Author = {B. Braida and P. C. Hiberty}, - Journal = {J. Phys. Chem. A}, - Pages = {13045}, - Volume = {112}, - Year = {2008}} - -@article{BraTouCafUmr-JCP-11, - Author = {B. Bra\"ida and J. Toulouse and M. Caffarel and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {084108}, - Title = {Quantum Monte Carlo with Jastrow-valence-bond wave functions}, - Volume = {134}, - Year = {2011}} - -@misc{BraTouCafUmr-JJJ-XX-note2, - Note = {In our BOVB wave functions, we use different sets of orbital coefficients, but a single set of basis exponents shared by all orbital sets.}} - -@misc{BraTouCafUmr-JJJ-XX-note3, - Note = {Bouab\c{c}a {\it et al.}~\cite{BouBraCaf-JCP-10} have introduced a wave function with several Jastrow factors attached to individual molecular orbitals. With such a wave function, the correlation effects can be treated differently in atomic and binding regions. In the case of the FH molecule, no atomic core Jastrow was used and two different valence Jastrow factors (one for the lone pairs paying a role in the bond and the other one for the $\sigma$-bond) were introduced. The resulting binding energy was essentially exact within error bars. Combining the various VB wave functions discussed in this work with this multi-Jastrow approach is presently under investigation.}} - -@misc{BraTouCafUmr-JJJ-XX-note, - Note = {In the condensed-matter community, ``stricly localized orbitals'' often refers to orbitals that vanish exactly at some finite distance. In the present work, ``stricly localized orbitals'' is employed in the sense usually used in the quantum chemistry community, i.e. orbitals expanded on Gaussian or Slater basis functions centered on a single atom. Thus, these orbitals vanish exactly only at infinite distance.}} - -@article{BreAda-JCP-11, - Author = {E. Br\'emond and C. Adamo}, - Journal = {J. Chem. Phys.}, - Pages = {024106}, - Volume = {135}, - Year = {2011}} - -@article{BreBou-PRB-96, - Author = {J. L. Bretonnet and M. Boulahbak}, - Journal = {Phys. Rev. B}, - Pages = {6859}, - Volume = {{53}}, - Year = {1996}} - -@incollection{BreCepRey-INC-01, - Author = {D. Bressanini and D. M. Ceperley and P. Reynolds}, - Booktitle = {Recent Advances in Quantum Monte Carlo Methods, II}, - Editor = {S. Rothstein}, - Publisher = {World Scientific}, - Title = {What do we know about wave function nodes?}, - Year = {2001}} - -@article{BreCioSanAda-ACR-16, - Author = {E. Br\'emond and I. Ciofini and J. C. Sancho-Garc\'ia and C. Adamo}, - Journal = {Acc. Chem. Res.}, - Pages = {1503}, - Volume = {49}, - Year = {2016}} - -@article{BreMelMor-PRA-98, - Author = {D. Bressanini and M. Mella and G. Morosi}, - Journal = {Phys. Rev. A}, - Pages = {1678}, - Volume = {57}, - Year = {1998}} - -@article{BreMorTar-JCP-05, - Author = {D. Bressanini and G. Morosi and S. Tarasco}, - Journal = {J. Chem. Phys.}, - Pages = {204109}, - Volume = {123}, - Year = {2005}} - -@article{BreSavPerSanAda-JCTC-18, - Author = {E. Br\'emond and M. Savarese and A. J. P\'erez-Jim\'enez and J. C. Sancho-Garc\'ia and C. Adamo}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4052}, - Volume = {14}, - Year = {2018}} - -@article{BroDevLem-PRB-80, - Author = {F. Brosens and J. T. Devreese and L. F. Lemmens}, - Journal = {Phys. Rev. B}, - Pages = {1363}, - Volume = {{21}}, - Year = {1980}} - -@article{BroPanSto-PRL-09, - Author = {Christian Brouder and Gianluca Panati and Gabriel Stoltz}, - Journal = {Phys. Rev. Lett.}, - Pages = {230401}, - Volume = {103}, - Year = {2009}} - -@article{BroTraLopNee-JCP-07, - Author = {M. D. Brown and J. R. Trail and P. L\'opez R\'ios and R. J. Needs}, - Journal = {J. Chem. Phys.}, - Pages = {224110}, - Title = {Energies of the first row atoms from quantum Monte Carlo}, - Volume = {126}, - Year = {2007}} - -@article{BroYinLor-SR-13, - Author = {V. Brosco and Z.-J. Ying and J. Lorenzana}, - Journal = {Sci. Rep.}, - Pages = {2172}, - Volume = {3}, - Year = {2013}} - -@article{BruHamNea-JCP-15, - Author = {F. Bruneval and S. M. Hamed and J. B. Neaton}, - Journal = {J. Chem. Phys.}, - Pages = {244101}, - Volume = {142}, - Year = {2015}} - -@article{BruProKroBre-JCP-17, - Author = {Iulia Emilia Brumboiu and Georgia Prokopiou and Leeor Kronik and Barbara Brena}, - Journal = {J. Chem. Phys.}, - Pages = {044301}, - Volume = {147}, - Year = {2017}} - -@phdthesis{Bru-THESIS-05, - Author = {F. Bruneval}, - School = {Ecole Polytechnique}, - Year = {2005}} - -@article{BuiBae-MP-02, - Author = {M. A. Buijse and E. J. Baerends}, - Journal = {Mol. Phys.}, - Pages = {401}, - Volume = {100}, - Year = {2002}} - -@article{BurCruLam-JCP-98, - Author = {K. Burke and F. G. Cruz and K.-C. Lam}, - Journal = {J. Chem. Phys}, - Pages = {8161}, - Volume = {109}, - Year = {1998}} - -@article{BurErnPer-CPL-97, - Author = {K. Burke and M. Ernzerhof and J. P. Perdew}, - Journal = {Chem. Phys. Lett.}, - Pages = {115}, - Volume = {265}, - Year = {1997}} - -@article{BurFilDol-JCP-07, - Author = {M. Burkatzki and C. Filippi and M. Dolg}, - Journal = {J. Chem. Phys.}, - Pages = {234105}, - Volume = {126}, - Year = {2007}} - -@article{Bur-JCP-12, - Author = {K. Burke}, - Journal = {J. Chem. Phys.}, - Pages = {150901}, - Title = {{Perspective on density functional theory}}, - Volume = {136}, - Year = {2012}} - -@article{BurPerErn-JCP-98, - Author = {K. Burke and J. P. Perdew and M. Ernzerhof}, - Journal = {J. Chem. Phys}, - Pages = {3760}, - Volume = {109}, - Year = {1998}} - -@article{BurPer-IJQC-95, - Author = {K. Burke and J. P. Perdew}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {199}, - Volume = {{56}}, - Year = {1995}} - -@article{BurPerLan-PRL-94, - Author = {K. Burke and J. P. Perdew and D. C. Langreth}, - Journal = {Phys. Rev. Lett.}, - Pages = {1283}, - Volume = {73}, - Year = {1994}} - -@article{BurPerLev-PRA-96, - Author = {K. Burke and J. P. Perdew and M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {R2915}, - Volume = {53}, - Year = {1996}} - -@inbook{BurPerWan-INC-98, - Address = {NY}, - Author = {Kieron Burke and John P. Perdew and Y. Wang}, - Booktitle = {Electronic Density Functional Theory: Recent Progress and New Directions}, - Date-Modified = {2013-02-12 00:16:04 +0000}, - Editor = {J. F. Dobson and G. Vignale and M. P. Das}, - Organization = {Plenum}, - Pages = {81}, - Pub-Num = {34}, - Publisher = {Plenum}, - Title = {Derivation of a generalized gradient approximation: The PW91 density functional}, - Url = {http://link.springer.com/chapter/10.1007%2F978-1-4899-0316-7_7}, - Year = {1997}, - Bdsk-Url-1 = {http://link.springer.com/chapter/10.1007%2F978-1-4899-0316-7_7}} - -@article{BygAllMan-JCP-12, - Author = {P. J. Bygrave and N. L. Allan and F. R. Manby}, - Journal = {J. Chem. Phys.}, - Pages = {164102}, - Volume = {137}, - Year = {2012}} - -@article{BylKle-PRB-90, - Author = {D. M. Bylander and L. Kleinman}, - Journal = {Phys. Rev. B}, - Pages = {7868}, - Volume = {41}, - Year = {1990}} - -@article{ByrCotMon-JCP-11, - Author = {{J. N. Byrd, R. C\^ot\'e, and J. A. Montgomery, Jr}}, - Journal = {J. Chem. Phys.}, - Pages = {244307}, - Volume = {135}, - Year = {2011}} - -@article{BytRue-JCP-05, - Author = {L. Bytautas and K. Ruedenberg}, - Journal = {J. Chem. Phys.}, - Pages = {154110}, - Volume = {122}, - Year = {2005}} - -@misc{BytRue-JCP-05-note, - Note = {Note that this estimate of the exact well depth differs from the one used in Ref.~\onlinecite{UmrTouFilSorHeg-JJJ-XX} where we used instead the scalar-relativistic, valence-corrected estimate of Ref.~\onlinecite{BytRue-JCP-05} since calculations were performed with a relativistic pseudopotential.}} - -@article{CadWah-ADNDT-74, - Author = {P. E. Cade and A. C. Wahl}, - Journal = {At. Data Nucl. Data Tables}, - Pages = {340}, - Volume = {13}, - Year = {1974}} - -@article{Caf-ActNum-98, - Author = {R. E. Caflisch}, - Journal = {Acta Numerica}, - Pages = {1}, - Title = {{Monte Carlo and quasi-Monte Carlo methods}}, - Volume = {1998}, - Year = {1998}} - -@article{CafCla-JCP-88, - Author = {M. Caffarel and P. Claverie}, - Doi = {10.1063/1.454228}, - Journal = {J. Chem. Phys.}, - Keywords = {QUANTUM STATISTICAL MECHANICS; MONTE CARLO METHOD; FERMIONS; FEYNMAN PATH INTEGRAL; SCHROEDINGER EQUATION}, - Number = {2}, - Pages = {1100-1109}, - Publisher = {AIP}, - Title = {{Development of a pure diffusion quantum Monte Carlo method using a full generalized Feynman--Kac formula. II. Applications to simple systems}}, - Volume = {88}, - Year = {1988}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.454228}} - -@article{CaiRei-JCP-00, - Author = {Z.-L. Cai and J. R. Reimers}, - Journal = {J. Chem. Phys.}, - Pages = {527}, - Volume = {112}, - Year = {2000}} - -@article{CaiZanKitKocKreScr-PRA-05, - Author = {J. Caillat and J. Zanghellini and M. Kitzler and O. Koch and W. Kreuzer and A. Scrinzi}, - Journal = {Phys. Rev. A}, - Pages = {012712}, - Volume = {71}, - Year = {2005}} - -@article{CalSor-PRB-98, - Author = {{M. Calandra Buonaura and S. Sorella}}, - Journal = {Phys. Rev. B}, - Pages = {11446}, - Title = {{Numerical study of the two-dimensional Heisenberg model using a Green function Monte Carlo technique with a fixed number of walkers}}, - Volume = {57}, - Year = {1998}} - -@article{CanBoyTha-JCP-93, - Author = {N. M. Cann and R. J. Boyd and A. J. Thakkar}, - Journal = {J. Chem. Phys.}, - Pages = {7132}, - Volume = {98}, - Year = {1993}} - -@article{CanMou-NL-14, - Author = {Eric Canc\`es and Nahia Mourad}, - Journal = {Nonlinearity}, - Number = {9}, - Pages = {1999}, - Title = {A mathematical perspective on density functional perturbation theory}, - Volume = {27}, - Year = {2014}} - -@article{CanPer-JCP-08, - Author = {E. Canc\`es and K. Pernal}, - Journal = {J. Chem. Phys.}, - Pages = {134108}, - Title = {{Projected gradient algorithms for Hartree-Fock and density matrix functional theory calculations}}, - Volume = {128}, - Year = {2008}} - -@article{CapNalPar-JCP-82, - Author = {Joseph F. Capitani and Roman F. Nalewajski and Robert G. Parr}, - Journal = {The Journal of Chemical Physics}, - Keywords = {MOLECULES; MOLECULAR STRAUCTURE; FUNCTIONALS; BORN–OPPENHEIMER APPROXIMATION; GROUND STATES; HAMILTONIANS; ELECTRON DENSITY; NUCLEI; ELECTRIC FIELDS; EXCITED STATES; BOUND STATE; USES}, - Number = {1}, - Pages = {568-573}, - Publisher = {AIP}, - Title = {Non-Born--Oppenheimer density functional theory of molecular systems}, - Url = {http://link.aip.org/link/?JCP/76/568/1}, - Volume = {76}, - Year = {1982}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/76/568/1}} - -@article{CarGod-JCP-88, - Author = {{E. A. Carter and W. A. Goddard III}}, - Journal = {J. Chem. Phys.}, - Pages = {3132}, - Volume = {88}, - Year = {1988}} - -@article{CarSilMet-JCP-79, - Author = {D. P. Carroll and H. J. Silverstone and R. M. Metzger}, - Journal = {J. Chem. Phys.}, - Pages = {4142}, - Volume = {71}, - Year = {1979}} - -@article{CarTruGag-JCTC-15, - Author = {R. K. Carlson and D. G. Truhlar and L. Gagliardi}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4077}, - Volume = {11}, - Year = {2015}} - -@article{CarTruGag-JPCA-17, - Author = {R. K. Carlson and D. G. Truhlar and L. Gagliardi}, - Journal = {J. Phys. Chem. A}, - Pages = {5540}, - Volume = {121}, - Year = {2017}} - -@article{CasAttSor-JCP-04, - Author = {Michele Casula and Claudio Attaccalite and Sandro Sorella}, - Journal = {J. Chem. Phys.}, - Pages = {7110}, - Title = {Correlated geminal wave function for molecules: An efficient resonating valence bond approach}, - Volume = {121}, - Year = {2004}} - -@article{CasGutGuaGadSalDau-JCP-00, - Author = {M. E. Casida and F. Gutierrez and J. Guan and F.-X. Gadea and D. Salahub and J.-P. Daudey}, - Journal = {J. Chem. Phys.}, - Pages = {7062}, - Volume = {113}, - Year = {2000}} - -@article{CasHui-ARPC-12, - Author = {M. E. Casida and M. Huix-Rotllant}, - Journal = {Annu. Rev. Phys. Chem.}, - Pages = {287}, - Title = {Progress in Time-Dependent Density-Functional Theory}, - Volume = {63}, - Year = {2012}} - -@incollection{CasHui-TCC-15, - Author = {M. E. Casida and M. Huix-Rotllant}, - Booktitle = {Density-Functional Methods for Excited States}, - Doi = {10.1007/128_2015_632}, - Editor = {N. Ferr\'e and M. Filatov and M. Huix-Rotllant}, - Publisher = {Springer}, - Series = {Topics in Current Chemistry}, - Year = {2015}, - Bdsk-Url-1 = {https://doi.org/10.1007/128_2015_632}} - -@incollection{Cas-INC-95, - Address = {Singapore}, - Author = {M. E. Casida}, - Booktitle = {Recent Advances in Density Functional Methods, Part I}, - Editor = {D. P. Chong}, - Pages = {155}, - Publisher = {World Scientific}, - Year = {1995}} - -@article{CasJamCasSal-JCP-98, - Author = {M. E. Casida and C. Jamorski and K. C. Casida and D. R. Salahub}, - Journal = {J. Chem. Phys.}, - Pages = {4439}, - Volume = {108}, - Year = {1998}} - -@article{Cas-JCP-05, - Author = {M. E. Casida}, - Journal = {J. Chem. Phys.}, - Pages = {054111}, - Volume = {122}, - Year = {2005}} - -@article{Cas-JCP-18, - Author = {D. Casanova}, - Journal = {J. Chem. Phys.}, - Pages = {124118}, - Volume = {148}, - Year = {2018}} - -@article{Cas-JMS-09, - Author = {M. E. Casida}, - Journal = {J. Mol. Struct.: THEOCHEM}, - Pages = {3}, - Volume = {914}, - Year = {2009}} - -@article{CasMelRap-JCP-03, - Author = {M. Casalegno and M. Mella and A. M. Rappe}, - Journal = {J. Chem. Phys.}, - Pages = {7193}, - Volume = {118}, - Year = {2003}} - -@article{CasPol-PR-48, - Author = {H. B. G. Casimir and D. Polder}, - Journal = {Phys. Rev.}, - Pages = {360}, - Volume = {73}, - Year = {1948}} - -@article{Cas-PRA-95, - Author = {M. E. Casida}, - Journal = {Phys. Rev. A}, - Pages = {2005}, - Volume = {51}, - Year = {1995}} - -@article{Cas-PRB-99, - Author = {M. E. Casida}, - Journal = {Phys. Rev. B}, - Pages = {4694}, - Volume = {59}, - Year = {1999}} - -@article{CasSal-JCP-00, - Author = {M. E. Casida and D. R. Salahub}, - Journal = {J. Chem. Phys.}, - Pages = {8918}, - Volume = {113}, - Year = {2000}} - -@article{CasSor-JCP-03, - Author = {M. Casula and S. Sorella}, - Journal = {J. Chem. Phys.}, - Pages = {6500}, - Volume = {119}, - Year = {2003}} - -@article{CatPicSamVan-PRB-96, - Author = {{F. Catara, G. Piccitto, M. Sambataro, and N. Van Giai}}, - Journal = {Phys. Rev. B}, - Pages = {17536}, - Volume = {54}, - Year = {1996}} - -@article{CemSonMoGao-JCTC-09, - Author = {A. Cembram and L. Song and Y. Mo and J. Gao}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2702}, - Volume = {5}, - Year = {2009}} - -@article{CepAld-PRL-80, - Author = {D. M. Ceperley and B. J. Alder}, - Journal = {Phys. Rev. Lett.}, - Pages = {566}, - Volume = {45}, - Year = {1980}} - -@article{CepBer-JCP-88, - Author = {D. M. Ceperley and B. Bernu}, - Journal = {J. Chem. Phys.}, - Pages = {6316}, - Volume = {89}, - Year = {1988}} - -@article{CepCheKal-PRB-77, - Author = {D. Ceperley and G. V. Chester and M. H. Kalos}, - Journal = {Phys. Rev. B}, - Pages = {3081}, - Title = {{Monte Carlo simulation of a many-fermion study}}, - Volume = {{16}}, - Year = {1977}} - -@article{Cep-JSP-86, - Author = {D. M. Ceperley}, - Journal = {J. Stat. Phys.}, - Pages = {815}, - Volume = {43}, - Year = {1986}} - -@article{Cep-JSP-91, - Author = {D. M. Ceperley}, - Journal = {J. Stat. Phys.}, - Pages = {1237}, - Title = {{Fermion nodes}}, - Volume = {63}, - Year = {1991}} - -@incollection{CepKal-INC-79, - Address = {Berlin}, - Author = {D. M. Ceperley and M. H. Kalos}, - Booktitle = {Monte Carlo Methods in Statistical Physics}, - Editor = {K. Binder}, - Pages = {145-194}, - Publisher = {Springer}, - Title = {Quantum Many-Body Problem}, - Year = {1979}} - -@article{CerHob-PCCP-05, - Author = {J. {\v C}ern{\'y} and P. Hobza}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {1624}, - Volume = {7}, - Year = {2005}} - -@phdthesis{Cer-THESIS-12, - Author = {O. \v{C}ert\'ik}, - School = {University of Nevada, Reno}, - Title = {Physics in Screening Environments}, - Year = {2012}} - -@article{ChaCio-JCP-94, - Author = {M. Challacombe and J. Cioslowski}, - Journal = {J. Chem. Phys.}, - Pages = {464}, - Volume = {100}, - Year = {1994}} - -@article{ChaGoeRad-JCC-16, - Author = {B. Chan and L. Goerigk and L. Radom}, - Journal = {J. Comput. Chem.}, - Pages = {183}, - Volume = {37}, - Year = {2016}} - -@article{ChaGor-JCP-09, - Author = {jeng-Da Chai and Martin Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {174105}, - Title = {Long-range corrected double-hybrid density functinals}, - Volume = {131}, - Year = {2009}} - -@article{ChaGre-JCP-72, - Author = {T. C. Chang and F. Grein}, - Journal = {J. Chem. Phys.}, - Pages = {5270}, - Volume = {57}, - Year = {1972}} - -@article{ChaGwaDavParFro-PRA-93, - Author = {S. J. Chakravorty and S. R. Gwaltney and E. R. Davidson and F. A. Parpia and C. Froese Fischer}, - Journal = {Phys. Rev. A}, - Pages = {3649}, - Title = {Ground-state correlation energies for atomic ions with 3 to 18 electrons}, - Volume = {{47}}, - Year = {1993}} - -@article{ChaHan-PRA-99, - Author = {G. Kin-Lic Chan and N. C. Handy}, - Journal = {Phys. Rev. A}, - Pages = {3075}, - Title = {Optimized Lieb-Oxford bound for the exchange-correlation energy}, - Volume = {{59}}, - Year = {1999}} - -@article{ChaHea-JCP-08, - Author = {J.-D. Chai and M. Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {084106}, - Volume = {128}, - Year = {2008}} - -@article{ChaHea-JCP-09, - Author = {J. Chai and M. Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {174105}, - Volume = {131}, - Year = {2009}} - -@article{ChaHea-PCCP-08, - Author = {Jeng-Da Chai and Martin Head-Gordon}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {6615}, - Volume = {10}, - Year = {2008}} - -@article{ChaJacAdaStoLei-JCP-10, - Author = {Sylvain Chabbal and Denis Jacquemin and Carlo Adamo and Hermann Stoll and Thierry Leininger}, - Journal = {J. Chem. Phys.}, - Pages = {151104}, - Title = {Bond length alternation of conjugated oligomers: Another step on the fifth rung of Perdew's ladder of functional}, - Volume = {133}, - Year = {2010}} - -@article{Cha-JCP-12, - Author = {J.-D. Chai}, - Journal = {J. Chem. Phys.}, - Pages = {154104}, - Title = {Density functional theory with fractional orbital occupations}, - Volume = {136}, - Year = {2012}} - -@article{Cha-JCP-99, - Author = {G. K.-L. Chan}, - Journal = {J. Chem. Phys.}, - Pages = {4710}, - Volume = {110}, - Year = {1999}} - -@article{ChaMao-CPL-12, - Author = {Jeng-Da Chai and Shan-Ping Mao}, - Journal = {Chem. Phys. Lett.}, - Pages = {121}, - Volume = {538}, - Year = {2012}} - -@misc{Cha-PROG-XX, - Note = {CHAMP, a quantum Monte Carlo program written by C. J. Umrigar, C. Filippi and J. Toulouse, \url{http://pages.physics.cornell.edu/~cyrus/champ.html}}} - -@article{ChaStoWerLei-MP-10, - Author = {Sylvain Chabbal and Hermann Stoll and Hans-Joachim Werner and Thierry Leininger}, - Journal = {Mol. Phys.}, - Pages = {3373}, - Title = {Analytic gradients for the combined sr-DFT/lr-MP2 method: application to weakly bound systems}, - Volume = {108}, - Year = {2010}} - -@article{CheMusAngRei-CPL-12, - Author = {E. Chermak and B. Mussard and J. G. \'Angy\'an and P. Reinhardt}, - Journal = {Chem. Phys. Lett.}, - Pages = {162}, - Volume = {550}, - Year = {2012}} - -@article{ChenWu-JPCA-09, - Author = {Z. Chen and J. Song and S. Shaik and P. C. Hiberty and W. Wu}, - Journal = {J. Phys. Chem. A}, - Pages = {11560}, - Volume = {113}, - Year = {2009}} - -@article{ChuChe-JCC-11, - Author = {Y.-Y. Chuang and S.-M. Chen}, - Journal = {J. Comput. Chem.}, - Pages = {1671}, - Volume = {32}, - Year = {2011}} - -@article{ChuDal-JCP-04, - Author = {X. Chu and A. Dalgarno}, - Journal = {J. Chem. Phys.}, - Pages = {4083}, - Volume = {121}, - Year = {2004}} - -@article{CioLiu-JCP-96a, - Author = {J. Cioslowski and G. Liu}, - Journal = {J. Chem. Phys.}, - Pages = {4151}, - Volume = {105}, - Year = {1996}} - -@article{CioLiu-JCP-96b, - Author = {J. Cioslowski and G. Liu}, - Journal = {J. Chem. Phys.}, - Pages = {8187}, - Volume = {105}, - Year = {1996}} - -@article{CioLiu-JCP-98, - Author = {J. Cioslowski and G. Liu}, - Journal = {J. Chem. Phys.}, - Pages = {8225}, - Volume = {109}, - Year = {1998}} - -@article{CioLiu-JCP-99, - Author = {J. Cioslowski and G. Liu}, - Journal = {J. Chem. Phys.}, - Pages = {1882}, - Volume = {110}, - Year = {1999}} - -@article{CioSteTanUmr-JCP-95, - Author = {Jerzy Cioslowski and Boris B. Stefanov and Agnes Tan and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {6093}, - Volume = {103}, - Year = {1995}} - -@article{CizPal-JCP-67, - Author = {J. {\v C}i{\v z}ek and J. Paldus}, - Journal = {J. Chem. Phys.}, - Pages = {3976}, - Volume = {47}, - Year = {1967}} - -@article{CizPal-JCP-70, - Author = {J. {\v C}i{\v z}ek and J. Paldus}, - Journal = {J. Chem. Phys.}, - Pages = {821}, - Volume = {53}, - Year = {1970}} - -@article{CizPal-PRA-71, - Author = {J. {\v C}i{\v z}ek and J. Paldus}, - Journal = {Phys. Rev. A}, - Pages = {525}, - Volume = {3}, - Year = {1971}} - -@incollection{Cla-INC-79, - Address = {Oxford}, - Author = {J.W. Clark}, - Booktitle = {Progress in Nuclear and Particle Physics Vol. 2}, - Editor = {D. H. Wilkinson}, - Pages = {89}, - Publisher = {Pergamon}, - Title = {Variational Theory of Nuclear Matter}, - Year = {1979}} - -@article{ClaMorMcmKimScu-JCP-11, - Author = {B. K. Clark and M. A. Morales and J. McMinis and J. Kim and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {244105}, - Title = {{Computing the energy of a water molecule using multideterminants: A simple, efficient algorithm}}, - Volume = {135}, - Year = {2011}} - -@article{CleRoe-ADNDT-74, - Author = {E. Clementi and C. Roetti}, - Journal = {At. Data Nucl. Data Tables}, - Pages = {177}, - Volume = {14}, - Year = {1974}} - -@article{CleVei-JCP-66, - Author = {E. Clementi and A. Veillard}, - Journal = {J. Chem. Phys.}, - Pages = {3050}, - Volume = {{44}}, - Year = {1966}} - -@article{CocAssLupTou-JCP-17, - Author = {E. Coccia and R. Assaraf and E. Luppi and J. Toulouse}, - Doi = {10.1063/1.4991563}, - Journal = {J. Chem. Phys.}, - Pages = {014106}, - Title = {Ab initio lifetime correction to scattering states for time-dependent electronic-structure calculations with incomplete basis sets}, - Volume = {147}, - Year = {2017}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.4991563}} - -@article{CocCheBarSorGui-JCTC-12, - Author = {E. Coccia and O. Chernomor and M. Barborini and S. Sorella and L. Guidoni}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1952}, - Title = {Molecular Electrical Properties from Quantum Monte Carlo Calculations: Application to Ethyne}, - Volume = {8}, - Year = {2012}} - -@article{CocDra-PRB-15, - Author = {C. Cocchi and C. Draxl}, - Journal = {Phys. Rev. B}, - Pages = {205126}, - Volume = {92}, - Year = {2015}} - -@article{CocMusLabCaiTaiTouLup-IJQC-16, - Author = {E. Coccia and B. Mussard and M. Labeye and J. Caillat and R. Ta\"{\i}eb and J. Toulouse and E. Luppi}, - Doi = {10.1002/qua.25146}, - Journal = {Int. J. Quantum Chem.}, - Pages = {1120-1131}, - Title = {Gaussian continuum basis functions for calculating high-harmonic generation spectra}, - Volume = {116}, - Year = {2016}, - Bdsk-Url-1 = {https://doi.org/10.1002/qua.25146}} - -@article{CohMorYan-CR-12, - Author = {A. J. Cohen and P. Mori-S\'anchez and W. Yang}, - Journal = {Chem. Rev.}, - Pages = {289}, - Title = {Challenges for Density Functional Theory}, - Volume = {112}, - Year = {2012}} - -@article{CohMorYan-JCP-07b, - Author = {Aron J. Cohen and Paula Mori-S\'anchez and Weitao Yang}, - Journal = {J. Chem. Phys.}, - Pages = {034101}, - Volume = {127}, - Year = {2007}} - -@article{CohMorYan-JCP-07, - Author = {Aron J. Cohen and Paula Mori-S\'anchez and Weitao Yang}, - Journal = {J. Chem. Phys.}, - Pages = {191109}, - Volume = {126}, - Year = {2007}} - -@article{CohMorYan-JCP-08, - Author = {Aron J. Cohen and Paula Mori-S\'anchez and Weitao Yang}, - Journal = {J. Chem. Phys.}, - Pages = {121104}, - Volume = {129}, - Year = {2008}} - -@article{CohMorYan-JCTC-09, - Author = {A. J. Cohen and P. Mori-S\'anchez and W. Yang}, - Journal = {J. Chem. Theory Comput.}, - Pages = {786}, - Volume = {5}, - Year = {2009}} - -@article{CohMorYan-PRB-08, - Author = {Aron J. Cohen and Paula Mori-S\'anchez and Weitao Yang}, - Journal = {Phys. Rev. B}, - Pages = {115123}, - Volume = {77}, - Year = {2008}} - -@article{CohMorYan-SCI-08, - Author = {A. J. Cohen and P. Mori-S\'anchez and W. Yang}, - Journal = {Science}, - Pages = {792}, - Volume = {321}, - Year = {2008}} - -@misc{Col-ARX-06, - Author = {F. Colonna}, - Note = {\url{http://arxiv.org/abs/cs/0601035v1}}} - -@article{Col-IJQC-67, - Author = {A. J. Coleman}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {457}, - Volume = {1}, - Year = {1967}} - -@article{ColJolPoiAngJan-CPC-94, - Author = {F. Colonna and L.-H. Jolly and R. A. Poirier and J. G. \'Angy\'an and G. Jansen}, - Journal = {Comp. Phys. Comm.}, - Pages = {293}, - Volume = {81}, - Year = {1994}} - -@article{ColMaySav-JJJ-XX, - Author = {F. Colonna and D. Maynau and A. Savin}, - Journal = {???}, - Volume = {{}}} - -@article{ColMaySav-PRA-03, - Author = {F. Colonna and D. Maynau and A. Savin}, - Journal = {Phys. Rev. A}, - Number = {1}, - Pages = {012505}, - Publisher = {APS}, - Title = {Correlation energy per particle from the coupling-constant integration}, - Volume = {68}, - Year = {2003}} - -@article{ColSal-JCP-83, - Author = {Renato Colle and Oriano Salvetti}, - Journal = {J. Chem. Phys.}, - Pages = {1404}, - Title = {A general method for approximating the electronic correlation energy in molecules and solids}, - Volume = {79}, - Year = {1983}} - -@article{ColSal-JCP-90, - Author = {Renato Colle and Oriano Salvetti}, - Journal = {J. Chem. Phys.}, - Page = {534}, - Volume = {93}, - Year = {1990}} - -@article{ColSal-TCA-75, - Author = {R. Colle and O. Salvetti}, - Journal = {Theor. Chim. Acta}, - Pages = {329}, - Volume = {37}, - Year = {1975}} - -@article{ColSal-TCA-79, - Author = {R. Colle and O. Salvetti}, - Journal = {Theor. Chim. Acta}, - Pages = {55}, - Volume = {53}, - Year = {1979}} - -@article{ColSav-JCP-99, - Author = {F. Colonna and A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {2828}, - Title = {Correlation energies for some two- and four-electron systems along thhe adiabatic connection in density functional theory}, - Volume = {{110}}, - Year = {1999}} - -@book{ColYuk-BOOK-00, - Address = {New York}, - Author = {A. J. Coleman and V. I. Yukalov}, - Publisher = {Springer-Verlag}, - Title = {Reduced Density Matrices: Coulson's Challenge}, - Year = {2000}} - -@article{Con-JCP-64, - Author = {H. Conroy}, - Journal = {J. Chem. Phys.}, - Pages = {1331}, - Title = {{Molecular Schr\"odinger equation. II. Monte Carlo evaluation of integrals}}, - Volume = {{41}}, - Year = {1964}} - -@article{CooGerRai-CR-91, - Author = {D. L. Cooper and J. Gerratt and M. Raimondi}, - Journal = {Chem. Rev.}, - Pages = {929}, - Volume = {91}, - Year = {1991}} - -@book{Coo-INC-02, - Editor = {D. L. Cooper}, - Publisher = {Elsevier}, - Title = {Valence Bond Theory}, - Year = {2002}} - -@article{CooPou-TCA-77, - Author = {I. L. Cooper and C. N. M. Pounder}, - Journal = {Theoret. Chim. Acta}, - Pages = {51}, - Volume = {47}, - Year = {1978}} - -@article{CorDelOniPal-PRB-98, - Author = {Massimiliano Corradini and Rodolfo Del Sole and Giovanni Onida and and Maurizia Palummo}, - Journal = {Phys. Rev. B}, - Pages = {14569}, - Volume = {{57}}, - Year = {1998}} - -@article{CorFraTeaFro-MP-13, - Author = {Y. Cornaton and O. Franck and A. M. Teale and E. Fromager}, - Journal = {Mol. Phys.}, - Pages = {1275}, - Title = {Analysis of double-hybrid density functionals along the adiabatic connection}, - Volume = {111}, - Year = {2013}} - -@misc{CorFro-ARX-13, - Author = {Yann Cornaton and Emmanuel Fromager}, - Note = {\url{http://fr.arxiv.org/abs/1312.0409}}} - -@article{CorFro-IJQC-14, - Author = {Y. Cornaton and E. Fromager}, - Journal = {Int. J. Quantum Chem.}, - Pages = {1199}, - Volume = {114}, - Year = {2014}} - -@article{CorJouIpaCasFilVel-JCP-07, - Author = {F. Cordova and L. Joubert Doriol and A. Ipatov and M. E. Casida and C. Filippi and A. Vela}, - Journal = {J. Chem. Phys.}, - Pages = {164111}, - Volume = {127}, - Year = {2007}} - -@article{CorStoJenFro-PRA-13, - Author = {Y. Cornaton and A. Stoyanova and H. J. Aa. Jensen and E. Fromager}, - Journal = {Phys. Rev. A}, - Pages = {022516}, - Volume = {88}, - Year = {2013}} - -@article{CouNei-PPSL-61, - Author = {C. A. Coulson and A. H. Neilson}, - Journal = {Proc. Phys. Soc. London}, - Pages = {831}, - Volume = {78}, - Year = {1961}} - -@article{Cre-MP-01, - Author = {D. Cremer}, - Journal = {Mol. Phys.}, - Pages = {1899}, - Title = {Density functional theory: coverage of dynamic and non-dynamic electron correlation effects}, - Volume = {99}, - Year = {2001}} - -@article{Cre-WIRES-11, - Author = {D. Cremer}, - Journal = {WIREs Comput. Mol. Sci.}, - Note = {doi: 10.1002/wcms.58}, - Pages = {509}, - Title = {M{\o}ller-Plesset perturbation theory: from small molecule methods to methods for thousands of atoms}, - Volume = {1}, - Year = {2011}} - -@article{CruLamBur-JPCA-98, - Author = {Federico G. Cruz and Kin-Chung Lam and Kieron Burke}, - Journal = {J. Phys. Chem. A}, - Pages = {4911}, - Volume = {102}, - Year = {1998}} - -@misc{Crystalweb-PROG-XX, - Note = {\url{http://www.crystal.unito.it}}, - Title = {CRYSTAL, a general-purpose program for the study of crystalline solids}} - -@incollection{CsaTayYar-INC-71, - Author = {GY. Csanak and H.S. Taylor and Robert Yaris}, - Doi = {10.1016/S0065-2199(08)60363-2}, - Editor = {D.R. Bates and Immanuel Esterman}, - Issn = {0065-2199}, - Pages = {287}, - Publisher = {Academic Press}, - Series = {Adv. At. Mol. Phys.}, - Title = {Green's Function Technique in Atomic and Molecular Physics}, - Volume = {7}, - Year = {1971}, - Bdsk-Url-1 = {https://doi.org/10.1016/S0065-2199(08)60363-2}} - -@article{CuiBulJimHenScu-JCP-13, - Author = {Yao Cui and Ireneusz W. Bulik and Carlos A. Jim\'enez-Hoyos and Thomas M. Henderson and Gustavo E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {154107}, - Volume = {139}, - Year = {2013}} - -@article{CuiYan-MP-10, - Author = {G. Cui and W. Yang}, - Journal = {Mol. Phys.}, - Pages = {2745}, - Volume = {108}, - Year = {2010}} - -@article{CurRagRedPop-JCP-97, - Author = {L. A. Curtiss and K. Raghavachari and P. C. Redfern and J. A. Pople}, - Journal = {J. Chem. Phys.}, - Pages = {1063}, - Volume = {106}, - Year = {1997}} - -@article{CurRagTruPop-JCP-91, - Author = {L. A. Curtiss and K. Raghavachari and G. W. Trucks and J. A. Pople}, - Journal = {J. Chem. Phys.}, - Pages = {7221}, - Volume = {94}, - Year = {1991}} - -@article{DahLeeBar-IJQC-05, - Author = {{N. E. Dahlen, R. van Leeuwen, and U. Von Barth}}, - Journal = {Int. J. Quantum Chem.}, - Pages = {512-519}, - Title = {Variational energy functionals of the Green function tested on molecules}, - Volume = {101}, - Year = {2005}} - -@article{DahLeeBar-PRA-06, - Author = {{N. E. Dahlen, R. van Leeuwen, and U. von Barth}}, - Journal = {Phys. Rev. A}, - Pages = {012511}, - Volume = {73}, - Year = {2006}} - -@article{DahLee-JCP-05, - Author = {{N. E. Dahlen and R. van Leeuwen}}, - Journal = {J. Chem. Phys.}, - Pages = {164102}, - Volume = {122}, - Year = {2005}} - -@article{DahLee-PRL-07, - Author = {{N. E. Dahlen and R. van Leeuwen}}, - Journal = {Phys. Rev. Lett.}, - Pages = {153004}, - Volume = {98}, - Year = {2007}} - -@article{Dal-CPL-79, - Author = {E. Dalgaard}, - Journal = {Chem. Phys. Lett.}, - Pages = {559}, - Volume = {65}, - Year = {1979}} - -@article{DalJor-JCP-78, - Author = {E. Dalgaard and P. J{\o}rgensen}, - Journal = {J. Chem. Phys.}, - Pages = {3833}, - Volume = {{69}}, - Year = {1978}} - -@misc{Dal-PROG-01, - Author = {T. Helgaker and H. J. Aa. Jensen and P. Jorgensen and J. Olsen and K. Ruud and H. Agren and A. A. Auer and K. L. Bak and V. Bakken and O. Christiansen and S. Coriani and P. Dahle and E. K. Dalskov and T. Enevoldsen and B. Fernandez and C. H\"{a}ttig and K. Hald and A. Halkier and H. Heiberg and H. Hettema and D. Jonsson and S. Kirpekar and R. Kobayashi and H. Koch and K.V. Mikkelsen and P. Norman and M.J. Packer and T. B. Pedersen and T. A. Ruden and A. Sanchez and T. Saue and S. P. A. Sauer and B. Schimmelpfennig and K. O. Sylvester-Hvid and P. R. Taylor and O. Vahtras}, - Title = {DALTON, a molecular electronic structure program, Release 1.2 (2001)}} - -@misc{Dal-PROG-11, - Author = {C. Angeli and K. L. Bak and V. Bakken and O. Christiansen and R. Cimiraglia and S. Coriani and P. Dahle and E. K. Dalskov and T. Enevoldsen and B. Fernandez and L. Ferrighi and L. Frediani and C. H\"{a}ttig and K. Hald and A. Halkier and H. Heiberg and T. Helgaker and H. Hettema and B. Jansik and H. J. Aa. Jensen and D. Jonsson and P. J\{\o}rgensen and S. Kirpekar and W. Klopper and S. Knecht and R. Kobayashi and J. Kongsted and H. Koch and A. Ligabue and O. B. Lutn{\ae}s and K. V. Mikkelsen and C. B. Nielsen and P. Norman and J. Olsen and A. Osted and M. J. Packer and T. B. Pedersen and Z. Rinkevicius and E. Rudberg and T. A. Ruden and K. Ruud and P. Salek and C. C. M. Samson and A. Sanchez de Meras and T. Saue and S. P. A. Sauer and B. Schimmelpfennig and A. H. Steindal and K. O. Sylvester-Hvid and P. R. Taylor and O. Vahtras and D. J. Wilson and H.{\AA}gren}, - Title = {DALTON, a molecular electronic structure program, Release DALTON2011 (2011), see http://daltonprogram.org}} - -@misc{Dalshort-PROG-11, - Title = {DALTON, a molecular electronic structure program, Release Dalton2011 (2011), see \url{http://daltonprogram.org}}} - -@misc{Dalshort-PROG-13, - Title = {{DALTON, a molecular electronic structure program, Release DALTON2013.0 (2013), see http://daltonprogram.org}}} - -@article{Dalton-WIRES-13, - Author = {{K. Aidas, C. Angeli, K. L. Bak, V. Bakken, R. Bast, L. Boman, O. Christiansen, R. Cimiraglia, S. Coriani, P. Dahle, et al.}}, - Journal = {WIREs Comput. Mol. Sci.}, - Note = {doi: 10.1002/wcms.1172}, - Title = {The Dalton quantum chemistry program system}, - Year = {2013}} - -@article{DanVos-PR-60, - Author = {E. Daniel and S. H. Vosko}, - Journal = {Phys. Rev.}, - Pages = {2041}, - Volume = {{120}}, - Year = {1960}} - -@article{DatDev-PJP-88, - Author = {S. N. Datta and G. Devaiah}, - Journal = {Pramana}, - Pages = {387}, - Volume = {30}, - Year = {1988}} - -@article{Dau-CPL-74, - Author = {J.-P. Daudey}, - Journal = {Chem. Phys. Lett.}, - Pages = {574}, - Volume = {24}, - Year = {1974}} - -@book{Dav-BOOK-76, - Address = {New York}, - Author = {E. R. Davidson}, - Publisher = {Academic Press}, - Title = {Reduced Density Matrices in Quantum Chemistry}, - Year = {1976}} - -@article{DavGriSto-JCP-72, - Author = {B. Davies and R. Grimm and R. G. Storer}, - Journal = {J. Chem. Phys.}, - Pages = {538-544}, - Volume = {9}, - Year = {1972}} - -@article{DavHagChaMeiFro-PRA-91, - Author = {E. R. Davidson and S. A. Hagstrom and S. J. Chakravorty and V. Meiser Umar and C. Froese Fischer}, - Journal = {Phys. Rev. A}, - Pages = {7071}, - Title = {Ground-state correlation energies for two- to ten-electron atomic ions}, - Volume = {{44}}, - Year = {1991}} - -@article{Dav-IJQC-98, - Author = {E. R. Davidson}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {241}, - Title = {How Robust is Present-Day DFT}, - Volume = {{69}}, - Year = {1998}} - -@article{DavPolAsgTos-PRB-02, - Author = {B. Davoudi and M. Polini and R. Asgari and M. P. Tosi}, - Journal = {Phys. Rev. B}, - Pages = {075110}, - Title = {Self-consistent Overhauser model for the pair distribution function of an electron gas in dimensionalities D=3 and D=2}, - Volume = {{66}}, - Year = {2002}} - -@article{DelGor-JCP-01, - Author = {{F. Della Sala and A. G\"orling}}, - Journal = {J. Chem. Phys.}, - Pages = {5718}, - Volume = {115}, - Year = {2001}} - -@article{DerPorBab-ADNDT-10, - Author = {A. Derevianko and S. G. Porsev and J. F. Babb}, - Journal = {At. Data Nucl. Data Tables}, - Pages = {323}, - Volume = {96}, - Year = {2010}} - -@article{DevBroLem-PRB-80, - Author = {J. T. Devreese and F. Brosens and L. F. Lemmens}, - Journal = {Phys. Rev. B}, - Pages = {1349}, - Volume = {{21}}, - Year = {1980}} - -@article{DewKel-JCE-71, - Author = {M. J. S. Dewar and J. Kelemen}, - Journal = {J. Chem. Educ.}, - Pages = {494}, - Volume = {48}, - Year = {1971}} - -@article{DeyPetWil-JPCA-07, - Author = {Nathan J. DeYonker and Kirk A. Peterson and Angela K. Wilson}, - Journal = {J. Phys. Chem. A}, - Pages = {11383}, - Volume = {111}, - Year = {2007}} - -@book{Dic-BOOK-12, - Address = {New York}, - Author = {Rainer Dick}, - Publisher = {Springer}, - Title = {Advanced Quantum Mechanics -- Materials and Photons}, - Year = {2012}} - -@article{Die-PRA-08, - Author = {D. J. Diestler}, - Journal = {Phys. Rev. A}, - Pages = {033814}, - Volume = {78}, - Year = {2008}} - -@article{DioRydSchLan-PRL-04, - Author = {M. Dion and H. Rydberg and E. Schr\"oder and D. C. Langreth and B. I. Lundqvist}, - Journal = {Phys. Rev. Lett.}, - Pages = {246401}, - Volume = {92}, - Year = {2004}} - -@article{Dir-PCPRS-30, - Author = {P. A. M. Dirac}, - Journal = {Proc. Cambridge Phil. Soc.}, - Pages = {376}, - Volume = {26}, - Year = {1930}} - -@article{DisLilTka-PNAS-12, - Author = {DiStasio, Robert A. and von Lilienfeld, O. Anatole and Tkatchenko, Alexandre}, - Doi = {10.1073/pnas.1208121109}, - Journal = {Proc. Natl. Acad. Sci.}, - Number = {37}, - Pages = {14791-14795}, - Title = {Collective many-body van der Waals interactions in molecular systems}, - Volume = {109}, - Year = {2012}, - Bdsk-Url-1 = {https://doi.org/10.1073/pnas.1208121109}} - -@article{DixClaLebRoc-JCTC-17, - Author = {A. Dixit and J. Claudot and S. Leb\`egue and D. Rocca}, - Journal = {J. Chem. Theory Comput.}, - Pages = {5432}, - Volume = {13}, - Year = {2017}} - -@article{DmiPei-IJQC-81, - Author = {Y. Dmitriev and G. Peinel}, - Journal = {Int. J. Quantum Chem.}, - Pages = {763}, - Volume = {19}, - Year = {1981}} - -@article{DobDin-PRL-96, - Author = {J. F. Dobson and Bradley P. Dinte}, - Journal = {Phys. Rev. Lett.}, - Pages = {1780}, - Volume = {76}, - Year = {1996}} - -@article{DobGou-JPCM-12, - Author = {J. F. Dobson and T. Gould}, - Journal = {J. Phys.: Condens. Matter}, - Pages = {073201}, - Volume = {24}, - Year = {2012}} - -@incollection{Dob-INC-94, - Address = {New York}, - Author = {J. F. Dobson}, - Booktitle = {Topics in Condensed Matter Physics}, - Editor = {M. P. Das}, - Note = {(Available also: arXiv:cond-mat/0311371)}, - Pages = {121-142}, - Publisher = {Nova Science Publishers}, - Year = {1994}} - -@article{Dob-JCTN-09, - Author = {J. F. Dobson}, - Journal = {J. Comput. Theor. Nanosci.}, - Pages = {960}, - Volume = {6}, - Year = {2009}} - -@article{DobMcLRubWanGouLeDin-AJC-01, - Author = {J F. Dobson and K. McLennan and A. Rubio and J. Wang and T. Gould and H. M. Le and B. P. Dinte}, - Journal = {Aust. J. Chem.}, - Pages = {513}, - Volume = {54}, - Year = {2001}} - -@article{DobWanDinMclLe-IJQC-05, - Author = {J. F. Dobson and J. Wang and B. P. Dinte and K. McLennan and H. M. Le}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {579}, - Volume = {101}, - Year = {2005}} - -@article{DobWan-PRB-00, - Author = {J. F. Dobson and J. Wang}, - Journal = {Phys. Rev. B}, - Pages = {10038}, - Volume = {62}, - Year = {2000}} - -@article{DolEstSer-JFA-00, - Author = {J. Dolbeault and M. J. Esteban and E. S\'er\'e}, - Journal = {J. Funct. Anal.}, - Pages = {208}, - Volume = {174}, - Year = {2000}} - -@article{DolKno-JCSFT-97, - Author = {N. L. Doltsinis and P. J. Knowles}, - Journal = {J. Chem. Soc., Faraday Trans.}, - Pages = {2025}, - Volume = {93}, - Year = {1997}} - -@article{DomBraLes-JPCA-08, - Author = {{D. Domin, B. Braida and W. A. Lester, Jr.}}, - Journal = {J. Chem. Phys. A}, - Pages = {8964}, - Volume = {112}, - Year = {2008}} - -@article{DomMulDalLisDieKla-TCA-04, - Author = {{S. A. do Monte, T. M\"uller, M. Dallos, H. Lischka, M. Diedenhofen, and A. Klamt}}, - Journal = {Theor. Chem. Acc.}, - Pages = {78}, - Volume = {111}, - Year = {2004}} - -@article{DomTayGil-JPC-96, - Author = {Jeremy P. Dombroski and Stephen W. Taylor and Peter M. W. Gill}, - Journal = {J. Phys. Chem.}, - Pages = {6272}, - Volume = {100}, - Year = {1996}} - -@article{DouRabLoo-JCP-55, - Author = {J. E. Douglas and B. S. Rabinovitch and F. S. Looney}, - Journal = {J. Chem. Phys.}, - Pages = {315}, - Title = {Kinetics of the Thermal Cis-Trans Isomerization of Dideuteroethylene}, - Volume = {23}, - Year = {1955}} - -@article{Dra-JPB-81, - Author = {R. J. Drachman}, - Journal = {J. Phys. B}, - Pages = {2733}, - Volume = {14}, - Year = {1981}} - -@book{DreGro-BOOK-90, - Address = {Berlin}, - Author = {R. M. Dreizler and E. K. U. Gross}, - Publisher = {Springer-Verlag}, - Title = {Density Functional Theory}, - Year = {1990}} - -@article{DreKin-JCP-94, - Author = {P. R. Dressel and F. W. King}, - Journal = {J. Chem. Phys.}, - Pages = {7515}, - Volume = {100}, - Year = {1994}} - -@article{DreWeiHea-JCP-03, - Author = {A. Dreuw and J. L. Weisman and M. Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {2943}, - Volume = {119}, - Year = {2003}} - -@article{DruWilNeeGal-PRL-05, - Author = {N. D. Drummond and A. J. Williamson and R. J. Needs and G. Galli}, - Journal = {Phys. Rev. Lett.}, - Pages = {096801}, - Volume = {95}, - Year = {2005}} - -@misc{DubEliVisBasSau-JJJ-XX, - Author = {S. Dubillard and E. Eliav and L. Visscher and R. Bast and T. Saue}, - Note = {unpublished}} - -@misc{DubEliVisBasSau-JJJ-XX_fr, - Author = {S. Dubillard and E. Eliav and L. Visscher and R. Bast and T. Saue}, - Note = {non publi{\'e}}} - -@article{DucBla-PRB-13, - Author = {I. Duchemin and X. Blase}, - Journal = {Phys. Rev. B}, - Pages = {245412}, - Volume = {87}, - Year = {2013}} - -@article{DucDeuBla-PRL-12, - Author = {I. Duchemin and T. Deutsch and X. Blase}, - Journal = {Phys. Rev. Lett.}, - Pages = {167801}, - Volume = {109}, - Year = {2012}} - -@article{DucDie-JCP-94, - Author = {W. Duch and G. H. F. Diercksen}, - Journal = {J. Chem. Phys.}, - Pages = {3018}, - Volume = {101}, - Year = {1994}} - -@article{Dun-JCP-89, - Author = {Thom H. Dunning}, - Journal = {J. Chem. Phys.}, - Pages = {1007}, - Title = {Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen}, - Volume = {90}, - Year = {1989}} - -@article{DunMei-JCP-83, - Author = {B. I. Dunlap and W. N. Mei}, - Journal = {J. Chem. Phys.}, - Number = {8}, - Pages = {4997}, - Title = {Basis set effects on spectroscopic constants for C[sub 2] and Si[sub 2] and the symmetry dilemma in the X alpha model}, - Volume = {78}, - Year = {1983}} - -@article{DupRysKin-JCP-76, - Author = {Michel Dupuis and John Rys and Harry F. King}, - Journal = {The Journal of Chemical Physics}, - Number = {1}, - Pages = {111-116}, - Publisher = {AIP}, - Title = {Evaluation of molecular integrals over Gaussian basis functions}, - Volume = {65}, - Year = {1976}} - -@phdthesis{Dwy-THESIS-11, - Address = {Durham}, - Author = {A. D. Dwyer}, - School = {Durham University}, - Title = {Weak interactions and excited states from Coulomb-attenuated DFT}, - Type = {{PhD thesis}}, - Year = {2011}} - -@article{EckPulWer-JCC-97, - Author = {F. Eckert and P. Pulay and H.-J. Werner}, - Journal = {J. Comput. Chem.}, - Pages = {1473}, - Volume = {18}, - Year = {1997}} - -@article{EggWeiRefShaDauBaeKumNeaZojKro-JCTC-14, - Author = {D. A. Egger and S. Weissman and S. Refaely-Abramson and S. Sharifzadeh and M. Dauth and R. Baer and S. K\"ummel and J. B. Neaton and E. Zojer and L. Kronik}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1934}, - Volume = {10}, - Year = {2014}} - -@article{EisLon-ZP-30, - Author = {R. Eisenschitz and F. London}, - Journal = {Z. Physik}, - Pages = {491}, - Volume = {60}, - Year = {1930}} - -@incollection{EllFurBur-INC-09, - Address = {NJ}, - Author = {Elliott, Peter and Furche, Filipp and Kieron Burke}, - Booktitle = {Reviews in Computational Chemistry}, - Editor = {K. B. Lipkowitz and T. R. Cundari}, - Pages = {91-165}, - Publisher = {Wiley, Hoboken}, - Title = {Excited states from time-dependent density functional theory}, - Year = {2009}} - -@article{EllGolCanMai-CP-11, - Author = {P. Elliot and S. Goldson and C. Canahui and N. T. Maitra}, - Journal = {Chem. Phys.}, - Pages = {110}, - Title = {{Perspectives on double-excitations in TDDFT}}, - Volume = {391}, - Year = {2011}} - -@article{Ell-JPB-77, - Author = {D. E. Ellis}, - Journal = {J. Phys. B,}, - Volume = {10}, - Year = {1977}} - -@article{ElsHobFraSuhKax-JCP-01, - Author = {M. Elstner and P. Hobza and T. Frauenheim and S. Suhai and E. Kaxiras}, - Journal = {J. Chem. Phys.}, - Pages = {5149}, - Volume = {114}, - Year = {2001}} - -@article{EmaGarRamLopFerMeiPal-JCC-03, - Author = {{I. Ema, J. M. Garc\'ia de la Vega, G. Ram\'irez, R. L\'opez, J. Fern\'andez Rico, H. Meissner and J. Paldus}}, - Journal = {J. Comput. Chem.}, - Pages = {859}, - Volume = {24}, - Year = {2003}} - -@article{EmaGarRamLopFerMeiPal-JCC-03_fr, - Author = {{I. Ema, J. M. Garc\'ia de la Vega, G. Ram\'irez, R. L\'opez, J. Fern\'andez Rico, H. Meissner et J. Paldus}}, - Journal = {J. Comput. Chem.}, - Pages = {859}, - Volume = {24}, - Year = {2003}} - -@article{EngBon-IJMPB-01, - Author = {E. Engel and A. F. Bonetti}, - Journal = {Int. J. Mod. Phys. B}, - Pages = {1703}, - Volume = {15}, - Year = {2001}} - -@article{EngDre-JCC-99, - Author = {E. Engel and R. M. Dreizler}, - Journal = {J. Comput. Chem.}, - Pages = {31}, - Volume = {20}, - Year = {1999}} - -@incollection{EngDre-TCC-96, - Address = {Berlin}, - Author = {E. Engel and R. M. Drezler}, - Booktitle = {Density-Functional Theory II, Topics in Current Chemistry Vol. 181}, - Editor = {R. F. Nalewajski}, - Pages = {1}, - Publisher = {Springer}, - Year = {1996}} - -@article{EngHocDre-PRA-00, - Author = {E. Engel and A. H\"ock and R. M. Dreizler}, - Journal = {Phys. Rev. A}, - Pages = {032502}, - Volume = {61}, - Year = {2000}} - -@incollection{Eng-INC-02, - Author = {E. Engel}, - Booktitle = {Relativistic Electronic Structure Theory, Part 1: Fundamentals}, - Editor = {P. Schwerdtfeger}, - Pages = {523-621}, - Publisher = {Elsevier}, - Series = {Theoretical and Computational Chemistry, Vol. 11}, - Year = {2002}} - -@incollection{Eng-INC-03, - Address = {Berlin}, - Author = {E. Engel}, - Booktitle = {A Primer in Density Functional Theory}, - Editor = {C. Fiolhais and F. Nogueira and M. A. L. Marques}, - Pages = {56-122}, - Publisher = {Springer}, - Series = {Vol. 620 of Lecture Notes in Physics}, - Year = {2003}} - -@article{EngJiaFac-PRA-05, - Author = {{E. Engel, H. Jiang, and A. Facco Bonetti}}, - Journal = {Phys. Rev. A}, - Pages = {052503}, - Volume = {72}, - Year = {2005}} - -@article{EngKelDre-PRA-96, - Author = {{E. Engel, S. Keller, and R. M. Dreizler}}, - Journal = {Phys. Rev. A}, - Pages = {1367}, - Volume = {53}, - Year = {1996}} - -@article{EngKelFacMulDre-PRA-95, - Author = {{E. Engel, S. Keller, A. Facco Bonetti, H. M\"uller, and R. M. Dreizler}}, - Journal = {Phys. Rev. A}, - Pages = {2750}, - Volume = {52}, - Year = {1995}} - -@incollection{EngMulSpeDre-INC-95, - Address = {New York}, - Author = {E. Engel and H. M\"uller and C. Speicher and R. M. Dreizler}, - Booktitle = {Density Functional Theory, Vol. 337 of NATO ASI Series B}, - Editor = {E. K. U. Gross and R. M. Dreizler}, - Pages = {65}, - Publisher = {Plenum}, - Year = {1995}} - -@article{Eng-PRA-95, - Author = {E. Engel}, - Journal = {Phys. Rev. A}, - Pages = {1159}, - Volume = {{51}}, - Year = {1995}} - -@article{EngVos-PRB-93, - Author = {E. Engel and S. H. Vosko}, - Journal = {Phys. Rev. B}, - Pages = {13164}, - Volume = {{47}}, - Year = {1993}} - -@article{ErhBleGor-PRL-16, - Author = {J. Erhard and P. Bleiziffer and A. G\"orling}, - Journal = {Phys. Rev. Lett.}, - Pages = {143002}, - Volume = {117}, - Year = {2016}} - -@article{ErnBurPer-JCP-96, - Author = {M. Ernzerhof and K. Burke and J. P. Perdew}, - Journal = {J. Chem. Phys.}, - Pages = {2798}, - Volume = {105}, - Year = {1996}} - -@article{Ern-CPL-96, - Author = {M. Ernzerhof}, - Journal = {Chem. Phys. Lett.}, - Pages = {499}, - Volume = {263}, - Year = {1996}} - -@article{ErnPerBur-IJQC-97, - Author = {M. Ernzerhof and J. P. Perdew and K. Burke}, - Journal = {Int. J. Quantum Chem.}, - Pages = {285}, - Volume = {64}, - Year = {1997}} - -@incollection{ErnPerBur-INC-96, - Address = {Berlin}, - Author = {M. Ernzerhof and J. P. Perdew, and K. Burke}, - Booktitle = {Density Functional Theory}, - Editor = {R. Nalewajski}, - Publisher = {Springer-Verlag}, - Year = {1996}} - -@article{ErnPer-JCP-98, - Author = {M. Ernzerhof and J. P. Perdew}, - Journal = {J. Chem. Phys.}, - Pages = {3313}, - Volume = {{109}}, - Year = {1998}} - -@article{ErnScu-JCP-99a, - Author = {M. Ernzerhof and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {5029}, - Volume = {110}, - Year = {1999}} - -@article{EshBatFur-TCA-12, - Affiliation = {Department of Chemistry, University of California, 1102 Natural Sciences II, Irvine, CA 92697-2025, USA}, - Author = {Eshuis, Henk and Bates, Jefferson and Furche, Filipp}, - Issue = {1}, - Journal = {Theor. Chem. Acc.}, - Keyword = {Chemistry and Materials Science}, - Optnote = {10.1007/s00214-011-1084-8}, - Opturl = {http://dx.doi.org/10.1007/s00214-011-1084-8}, - Pages = {1084}, - Publisher = {Springer Berlin / Heidelberg}, - Title = {Electron correlation methods based on the random phase approximation}, - Volume = {131}, - Year = {2012}} - -@article{EshFur-JCP-12, - Author = {H. Eshuis and F. Furche}, - Journal = {J. Chem. Phys.}, - Pages = {084105}, - Volume = {136}, - Year = {2012}} - -@article{EshFur-JPCL-11, - Author = {H. Eshuis and F. Furche}, - Journal = {J. Phys. Chem. Lett.}, - Pages = {983}, - Volume = {2}, - Year = {2011}} - -@article{EshYarFur-JCP-10, - Author = {Henk Eshuis and Julian Yarkony and Filipp Furche}, - Journal = {J. Chem. Phys.}, - Pages = {234114}, - Volume = {132}, - Year = {2010}} - -@article{EvaShuTul-JPCA-13, - Author = {F. A. Evangelista and P. Shushkov and J. C. Tully}, - Journal = {J. Phys. Chem. A}, - Pages = {7378}, - Volume = {117}, - Year = {2013}} - -@article{Ewa-AP-21, - Author = {P. P. Ewald}, - Journal = {Ann. Phys.}, - Pages = {253}, - Volume = {{64}}, - Year = {1921}} - -@misc{exp_2nd_excited_state, - Note = {Le r{\'e}sultat exp{\'e}rimental dans l'article de Alijah et Duxbury (1.411 eV) a {\'e}t{\'e} corrig{\'e} pour enlever l'{\'e}nergie de point z{\'e}ro en utilisant les calculs FCI/TZ2P de Sherrill et al. (0.004 eV).}} - -@article{FabBouDucAttBla-JCP-13, - Author = {C. Faber and P. Boulanger and I. Duchemin and C. Attaccalite and X. Blase}, - Journal = {J. Chem. Phys.}, - Pages = {194308}, - Volume = {139}, - Year = {2013}} - -@article{FabDel-JCP-07, - Author = {{E. Fabiano and F. Della Sala}}, - Journal = {J. Chem. Phys.}, - Pages = {214102}, - Volume = {126}, - Year = {2007}} - -@article{FabDel-TCA-12, - Author = {{E. Fabiano and F. Della Sala}}, - Journal = {Theor. Chem. Acc.}, - Pages = {1278}, - Volume = {131}, - Year = {2012}} - -@article{FabDucDeuBla-PRB-12, - Author = {C. Faber and I. Duchemin and T. Deutsch and X. Blase}, - Journal = {Phys. Rev. B}, - Pages = {155315}, - Volume = {86}, - Year = {2012}} - -@article{FacEngSchDre-PRL-01, - Author = {{A. Facco Bonetti, E. Engel, R. N. Schmid, and R. M. Dreizler}}, - Journal = {Phys. Rev. Lett.}, - Pages = {2241}, - Volume = {86}, - Year = {2001}} - -@article{FacEngSchDre-PRL-03, - Author = {{A. Facco Bonetti, E. Engel, R. N. Schmid, and R. M. Dreizler}}, - Journal = {Phys. Rev. Lett.}, - Pages = {219302}, - Volume = {90}, - Year = {2003}} - -@incollection{Fah-INC-99, - Address = {Dordrecht}, - Author = {S. Fahy}, - Booktitle = {Quantum Monte Carlo Methods in Physics and Chemistry}, - Editor = {M. P. Nightingale and C. J. Umrigar}, - Pages = {101}, - Publisher = {Kluwer}, - Series = {NATO ASI Ser. C 525}, - Year = {1999}} - -@article{FarHeiEngRob-PRB-93, - Author = {B. Farid and V. Heine and G. E. Engel and I. J. Robertson}, - Journal = {Phys. Rev. B}, - Pages = {11602}, - Volume = {{48}}, - Year = {1993}} - -@article{FasCorSanTru-JPCA-99, - Author = {P. L. Fast and J. Corchado and M. L. Sanchez and D. G. Truhlar}, - Journal = {J. Phys. Chem. A}, - Pages = {3139}, - Volume = {103}, - Year = {1999}} - -@article{FasSanTru-JCP-99, - Author = {P. L. Fast and M. L. S\'anchez and D. G. Truhlar}, - Journal = {J. Chem. Phys.}, - Pages = {2921}, - Volume = {111}, - Year = {1999}} - -@article{Fel-JCC-96, - Author = {D. Feller}, - Journal = {J. Comput. Chem.}, - Pages = {1571}, - Volume = {17}, - Year = {1996}} - -@article{Fel-JCP-13, - Author = {D. Feller}, - Journal = {J. Chem. Phys.}, - Pages = {074103}, - Volume = {138}, - Year = {2013}} - -@article{Fel-JCP-92, - Author = {D. Feller}, - Journal = {J. Chem. Phys.}, - Pages = {6104}, - Volume = {96}, - Year = {1992}} - -@article{Fel-JCP-93, - Author = {D. Feller}, - Journal = {J. Chem. Phys.}, - Pages = {7059}, - Volume = {98}, - Year = {1993}} - -@article{FelPetHil-JCP-10, - Author = {D. Feller and K. A. Peterson and J. G. Hill}, - Journal = {J. Chem. Phys.}, - Pages = {184102}, - Volume = {133}, - Year = {2010}} - -@article{FerAss-JCP-02, - Author = {N. Ferr\'e and X. Assfeld}, - Journal = {J. Chem. Phys.}, - Pages = {4119}, - Volume = {117}, - Year = {2002}} - -@article{FerBalLop-JCTC-15, - Author = {R. G. Fernando and M. C. Balhoff and K. Lopata}, - Journal = {J. Chem. Theory Comput.}, - Pages = {646}, - Volume = {11}, - Year = {2015}} - -@article{FerGinTou-JCP-19, - Author = {Anthony Fert\'e and Emmanuel Giner and Julien Toulouse}, - Doi = {10.1063/1.5082638}, - Journal = {J. Chem. Phys.}, - Pages = {084103}, - Title = {Range-separated multideterminant density-functional theory with a short-range correlation functional of the on-top pair density}, - Volume = {150}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5082638}} - -@article{FerLopAguEmaRam-IJQC-01, - Author = {{J. Fern\'andez Rico, R. L\'opez, A. Aguado, I. Ema, and G. Ram\'irez}}, - Journal = {Int. J. Quantum Chem.}, - Pages = {148}, - Volume = {81}, - Year = {2001}} - -@article{Fer-PR-57, - Author = {R. A. Ferrell}, - Journal = {Phys. Rev.}, - Pages = {450}, - Volume = {{107}}, - Year = {1957}} - -@article{FerRamLopFer-CCCC-88, - Author = {{J. Fern\'andez Rico, G. Ram\'irez, R. L\'opez and J. I. Fern\'andez-Alonso}}, - Journal = {Collection Czechoslovak Chem. Commun.}, - Pages = {2250}, - Volume = {{53}}, - Year = {1988}} - -@book{FetWal-BOOK-03, - Author = {A. L. Fetter and J. D. Walecka}, - Publisher = {Dover}, - Title = {Quantum Theory of Many-Particle Systems}, - Year = {2003}} - -@article{FilAssMor-JCP-16, - Author = {C. Filippi, R. Assaraf and S. Moroni}, - Journal = {J. Chem. Phys.}, - Pages = {194105}, - Title = {{Simple formalism for efficient derivatives and multi-determinant expansions in quantum Monte Carlo}}, - Volume = {144}, - Year = {2016}} - -@article{FilFah-JCP-00, - Author = {Claudia Filippi and Stephen Fahy}, - Journal = {J. Chem. Phys.}, - Pages = {3523}, - Volume = {112}, - Year = {2000}} - -@incollection{FilGonUmr-INC-96, - Address = {Amsterdam}, - Author = {Claudia Filippi and Xavier Gonze and C. J. Umrigar}, - Booktitle = {Recent Developments of Modern Density Functional Theory}, - Editor = {J. M. Seminario}, - Pages = {295-326}, - Publisher = {Elsevier}, - Title = {Generalized gradient approximations to density functional theory: comparison with exact results}, - Year = {1996}} - -@misc{Fil-PRIV-XX, - Author = {C. Filippi}, - Note = {private communication}} - -@article{FilSha-CPL-00, - Author = {Michael Filatov and Sason Shaik}, - Journal = {Chem. Phys. Lett.}, - Pages = {409}, - Volume = {332}, - Year = {1999}} - -@article{FilSha-CPL-99, - Author = {M. Filatov and S. Shaik}, - Journal = {Chem. Phys. Lett.}, - Pages = {429}, - Title = {{A spin-restricted ensemble-referenced Kohn-Sham method and its application to diradicaloid situations}}, - Volume = {304}, - Year = {1999}} - -@article{FilSha-JPCA-00, - Author = {Michael Filatov and Sason Shaik}, - Journal = {J. Phys. Chem. A}, - Pages = {6628}, - Volume = {104}, - Year = {2000}} - -@article{FilSha-JPCA-99, - Author = {Michael Filatov and Sason Shaik}, - Journal = {J. Phys. Chem. A}, - Pages = {8885}, - Volume = {103}, - Year = {1999}} - -@article{FilShaWoeGriPey-CPL-00, - Author = {Michael Filatov and Sason Shaik and M. Woeller and S. Grimme and S.D. Peyerimhoff}, - Journal = {Chem. Phys. Lett.}, - Pages = {135}, - Volume = {316}, - Year = {2000}} - -@misc{FilTouUmr-JJJ-XX, - Author = {Claudia Filippi and Julien Toulouse and C. J. Umrigar}, - Title = {in preparation}} - -@article{FilUmrGon-JCP-97, - Author = {C. Filippi and C. J. Umrigar and X. Gonze}, - Journal = {J. Chem. Phys.}, - Pages = {9994}, - Title = {{Excitation energies from density functional perturbation theory}}, - Volume = {107}, - Year = {1997}} - -@article{FilUmrGon-PRA-96, - Author = {C. Filippi and C. J. Umrigar and X. Gonze}, - Journal = {Phys. Rev. A}, - Pages = {4810}, - Volume = {54}, - Year = {1996}} - -@article{FilUmr-JCP-96, - Author = {C. Filippi and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {213}, - Title = {Multiconfiguration wave functions for quantum Monte Carlo calculations of first-row diatomic molecules}, - Volume = {{105}}, - Year = {1996}} - -@article{Fil-WIR-14, - Author = {M. Filatov}, - Journal = {WIREs Comput. Mol. Sci.}, - Pages = {146}, - Title = {{Spin-restricted ensemble-referenced Kohn-Sham method: basic principles and application to strongly correlated ground and excited states of molecules}}, - Volume = {5}, - Year = {2015}} - -@article{FilZacBud-JCTC-09, - Author = {C. Filippi and M. Zaccheddu and F. Buda}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2074}, - Title = {Absorption Spectrum of the Green Fluorescent Protein Chromophore: A Difficult Case for ab Initio Methods?}, - Volume = {5}, - Year = {2009}} - -@article{FilZacBud-JJJ-XX, - Author = {Claudia Filippi and Maurizio Zaccheddu and Francesco Buda}, - Note = {unpublished}} - -@incollection{FlaCafSav-INC-97, - Address = {Singapore}, - Author = {H.-J. Flad and M. Caffarel and A. Savin}, - Booktitle = {Recent advances in quantum Monte Carlo methods}, - Editor = {W. A. Lester}, - Pages = {73}, - Publisher = {World Scientific}, - Title = {Quantum Monte Carlo calculations with multi-reference trial wave functions}, - Year = {1997}} - -@misc{Fla-PRIV-XX, - Author = {H. J. Flad}, - Title = {private communication}} - -@article{FlaSav-JCP-95, - Author = {H.-J. Flad and A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {691}, - Volume = {103}, - Year = {1995}} - -@article{FlaSavPre-JCP-92, - Author = {H.-J. Flad and A. Savin and H. Preuss}, - Journal = {J. Chem. Phys.}, - Pages = {459}, - Volume = {97}, - Year = {1992}} - -@article{FlaSavScuNicPre-CPL-94, - Author = {H.-J. Flad and A. Savin and M. Schultheiss and A. Nicklass and H. Preuss}, - Journal = {Chem. Phys. Lett.}, - Pages = {274}, - Volume = {222}, - Year = {1994}} - -@article{FloGda-JCP-05, - Author = {J. R. Flores and R. J. Gdanitz}, - Journal = {J. Chem. Phys.}, - Pages = {144316}, - Volume = {123}, - Year = {2005}} - -@article{Foc-ZP-30, - Author = {V. Fock}, - Journal = {Z. Phys.}, - Pages = {855}, - Volume = {63}, - Year = {1930}} - -@article{FouMitNeeRaj-RMP-01, - Author = {W. M. C. Foulkes and L. Mitas and R. J. Needs and G. Rajagopal}, - Journal = {Rev. Mod. Phys.}, - Pages = {33}, - Title = {{Quantum Monte Carlo simulations of solids}}, - Volume = {{73}}, - Year = {2001}} - -@article{FraDurMes-JCP-97, - Author = {X. Fradera and M. Duran and J. Mestres}, - Journal = {J. Chem. Phys.}, - Pages = {3576}, - Volume = {107}, - Year = {1997}} - -@article{FraFilAmo-JCTC-12, - Author = {F. Fracchia and C. Filippi and C. Amovilli}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1943}, - Title = {Size-extensive wave functions for quantum Monte Carlo: A linear scaling generalized valence bond approach}, - Volume = {8}, - Year = {2012}} - -@misc{FraLupTou-JJJ-XX, - Author = {O. Franck and E. Luppi and J. Toulouse}, - Note = {unpublished}} - -@article{FraMusLupTou-JCP-15, - Author = {O. Franck and B. Mussard and E. Luppi and J. Toulouse}, - Journal = {J. Chem. Phys.}, - Pages = {074107}, - Title = {Basis convergence of range-separated density-functional theory}, - Volume = {142}, - Year = {2015}} - -@misc{FraMusLupTou-JJJ-XX, - Author = {O. Franck and B. Mussard and E. Luppi and J. Toulouse}, - Note = {Basis convergence of range-separated density-functional theory, arXiv:1412.2613, to appear in J. Chem. Phys.}} - -@misc{FraMusLupTou-JJJ-XX-note1, - Note = {Note that the partial-wave expansion of any {\it odd} power of $r_{12}$ contains an infinite number of terms. In contrast, the partial-wave expansion of any {\it even} power of $r_{12}$ terminates at a finite $\ell$.}} - -@misc{FraMusLupTou-JJJ-XX-note2, - Note = {For a discussion of angular and radial correlation and the shape of the correlation hole in the He atom with the long-range interaction, see Ref.~\onlinecite{PolColLeiStoWerSav-IJQC-03}.}} - -@misc{FraMusLupTou-JJJ-XX-note3, - Note = {For $\mu=1$ the difference between the long-range MP2 correlation energies for $X=5$ and $X=6$ is still as small as about 0.2 mhartree.}} - -@misc{FraMusLupTou-JJJ-XX-note4, - Note = {For $r_1=r_2$, $f\lr_\ell >0$ for $\ell=0$ and $f\lr_\ell <0$ for $\ell \geq 1$.}} - -@article{FreHuxMor-PRA-84, - Author = {{D. E. Freund, B. D. Huxtable, and J. D. Morgan III}}, - Journal = {Phys. Rev. A}, - Pages = {980}, - Volume = {29}, - Year = {1984}} - -@article{FreLev-JCP-82, - Author = {Karl F. Freed and Mel Levy}, - Journal = {The Journal of Chemical Physics}, - Keywords = {ALGORITHMS; ELECTRON DENSITY; FUNCTIONALS; SERIES EXPANSION; WAVE FUNCTIONS; GROUND STATES}, - Number = {1}, - Pages = {396-398}, - Publisher = {AIP}, - Title = {Direct first principles algorithm for the universal electron density functional}, - Url = {http://link.aip.org/link/?JCP/77/396/1}, - Volume = {77}, - Year = {1982}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/77/396/1}} - -@article{Fre-PRB-77, - Author = {D. L. Freeman}, - Journal = {Phys. Rev. B}, - Pages = {5512}, - Volume = {{15}}, - Year = {1977}} - -@article{FroCimJen-PRA-10, - Author = {E. Fromager and R. Cimiraglia and H. J. Aa. Jensen}, - Journal = {Phys. Rev. A}, - Pages = {024502}, - Volume = {81}, - Year = {2010}} - -@article{Fro-JCP-11, - Author = {E. Fromager}, - Journal = {J. Chem. Phys.}, - Pages = {244106}, - Volume = {135}, - Year = {2011}} - -@article{FroJen-JCP-11, - Author = {E. Fromager and H. J. Aa. Jensen}, - Journal = {J. Chem. Phys.}, - Pages = {034116}, - Volume = {135}, - Year = {2011}} - -@article{FroJen-PRA-08, - Author = {E. Fromager and H. J. Aa. Jensen}, - Journal = {Phys. Rev. A}, - Pages = {022504}, - Volume = {78}, - Year = {2008}} - -@misc{FroKneJen-ARX-12, - Author = {Emmanuel Fromager and Stefan Knecht and H. J. Aa. Jensen}, - Note = {\url{http://fr.arxiv.org/abs/1211.4829v1}}} - -@article{FroKneJen-JCP-13, - Author = {E. Fromager and S. Knecht and H. J. Aa. Jensen}, - Journal = {J. Chem. Phys.}, - Pages = {084101}, - Title = {{Multi-configuration time-dependent density-functional theory based on range separation}}, - Volume = {138}, - Year = {2013}} - -@article{FroReaWahWahJen-JCP-09, - Author = {E. Fromager and F. R\'eal and P. W{\aa}hlin and U. Wahlgren and H. J. Aa. Jensen}, - Journal = {J. Chem. Phys.}, - Pages = {054107}, - Volume = {131}, - Year = {2009}} - -@article{FroTouJen-JCP-07, - Author = {E. Fromager and J. Toulouse and H. J. Aa. Jensen}, - Journal = {J. Chem. Phys.}, - Pages = {074111}, - Title = {On the universality of the long-/short-range separation in multiconfigurational density-functional theory}, - Volume = {126}, - Year = {2007}} - -@article{FucGon-PRB-02, - Author = {M. Fuchs and X. Gonze}, - Journal = {Phys. Rev. B}, - Pages = {235109}, - Volume = {65}, - Year = {2002}} - -@article{FucNiqGonBur-JCP-05, - Abstract = {We show that density functional theory within the RPA (random phase - approximation for the exchange-correlation energy) provides a correct - description of bond dissociation in H2 in a spin-restricted Kohn-<96>Sham - formalism, i.e., without artificial symmetry breaking. We present - accurate adiabatic connection curves both at equilibrium and beyond - the Coulson-Fisher point. The strong curvature at large bond length - implies important static (left-<96>right) correlation, justifying modern - hybrid functional constructions but also demonstrating their limitations. - Although exact at infinite separation and accurate near the equilibrium - bond length, the RPA dissociation curve displays unphysical repulsion - at larger but finite bond lengths. Going beyond the RPA by including - the exact exchange kernel (RPA + X), we find a similar repulsion. - We argue that this deficiency is due to the absence of double excitations - in adiabatic linear response theory. Further analyzing the H2 dissociation - limit we show that the RPA + X is not size consistent, in contrast - to the RPA.}, - Author = {Fuchs, M. and Niquet, Y. M. and Gonze, X. and Burke, K.}, - Doi = {10.1063/1.1858371}, - Journal = {J. Chem. Phys.}, - Pages = {094116}, - Title = {Describing static correlation in bond dissociation by Kohn-Sham density functional theory}, - Volume = {122}, - Year = {2005}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.1858371}} - -@article{FukIwaSaw-PR-64, - Author = {N. Fukuda and F. Iwamoto and K. Sawada}, - Journal = {Phys. Rev.}, - Pages = {A932}, - Volume = {135}, - Year = {1964}} - -@book{Ful-BOOK-93, - Address = {Berlin}, - Author = {P. Fulde}, - Publisher = {Springer}, - Title = {Electron Correlations in Molecules and Solids}, - Year = {1993}} - -@article{Fur-JCP-01, - Author = {F. Furche}, - Journal = {J. Chem. Phys.}, - Pages = {5982}, - Volume = {114}, - Year = {2001}} - -@article{Fur-JCP-08, - Author = {F. Furche}, - Journal = {J. Chem. Phys.}, - Pages = {114105}, - Volume = {129}, - Year = {2008}} - -@article{FurPer-JCP-06, - Author = {F. Furche and J. P. Perdew}, - Journal = {J. Chem. Phys.}, - Pages = {044103}, - Volume = {124}, - Year = {2006}} - -@article{Fur-PRA-04, - Author = {Filipp Furche}, - Eid = {022514}, - Journal = {Physical Review A (Atomic, Molecular, and Optical Physics)}, - Keywords = {density functional theory; HF calculations; boson systems; electron pairs; ground states; Schrodinger equation}, - Number = {2}, - Numpages = {10}, - Pages = {022514}, - Publisher = {APS}, - Title = {Towards a practical pair density-functional theory for many-electron systems}, - Url = {http://link.aps.org/abstract/PRA/v70/e022514}, - Volume = {70}, - Year = {2004}, - Bdsk-Url-1 = {http://link.aps.org/abstract/PRA/v70/e022514}} - -@article{Fur-PRB-01, - Author = {F. Furche}, - Journal = {Phys. Rev. B}, - Pages = {195120}, - Volume = {64}, - Year = {2001}} - -@incollection{FurRap-INC-05, - Address = {Amsterdam}, - Author = {F. Furche and D. Rappoport}, - Booktitle = {Computational Photochemistry}, - Editor = {M. Olivucci}, - Pages = {93-128}, - Publisher = {Elsevier}, - Series = {Theoretical and Computational Chemistry, Vol. 16}, - Title = {Density functional methods for excited states: equilibrium structure and electronic spectra}, - Year = {2005}} - -@article{FurVoo-JCP-05, - Author = {F. Furche and T. Van Voorhis}, - Journal = {J. Chem. Phys.}, - Pages = {164106}, - Title = {Fluctuation-dissipation theorem density-functional theory}, - Volume = {122}, - Year = {2005}} - -@article{GagTruLiCarHoyBa-ACR-17, - Author = {{L. Gagliardi, D. G. Truhlar, G. Li Manni, R. K. Carlson, C. E. Hoyer, and J. Lucas Bao}}, - Journal = {Acc. Chem. Res.}, - Pages = {66}, - Volume = {50}, - Year = {2017}} - -@book{Gal-BOOK-02, - Author = {G. A. Gallup}, - Publisher = {Cambridge University Press}, - Title = {Valence Bond Methods: Theory and applications}, - Year = {2002}} - -@article{GalBueSar-CPL-03a, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {Chem. Phys. Lett.}, - Pages = {330}, - Volume = {378}, - Year = {2003}} - -@article{GalBueSar-CPL-03, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {Chem. Phys. Lett.}, - Pages = {327}, - Volume = {370}, - Year = {2003}} - -@article{GalBueSar-JCP-01, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {J. Chem. Phys.}, - Pages = {1166}, - Volume = {115}, - Year = {2001}} - -@article{GalBueSar-JCP-02, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {J. Chem. Phys.}, - Pages = {6071}, - Volume = {117}, - Year = {2002}} - -@article{GalBueSar-JCP-03, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {J. Chem. Phys.}, - Pages = {6858}, - Volume = {118}, - Year = {2003}} - -@article{GalBueSar-JCP-05a, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {J. Chem. Phys.}, - Pages = {034302}, - Volume = {123}, - Year = {2005}} - -@article{GalBueSar-JCP-05, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {J. Chem. Phys.}, - Pages = {154307}, - Volume = {122}, - Year = {2005}} - -@article{GalBueSar-JCP-99, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {J. Chem. Phys.}, - Pages = {10903}, - Volume = {111}, - Year = {1999}} - -@article{GalBueSar-PRA-00, - Author = {F. J. G\'alvez and E. Buend\'ia and A. Sarsa}, - Journal = {Phys. Rev. A}, - Pages = {052505}, - Volume = {61}, - Year = {2000}} - -@article{GalHanCohCha-CPL-05, - Author = {P. T. A. Galek and N. C. Handy and A. J. Cohen and G. K.-L. Chan}, - Journal = {Chem. Phys. Lett.}, - Pages = {156}, - Volume = {404}, - Year = {2005}} - -@article{GalHanLes-MP-06, - Author = {{P. T. A. Galek, N. C. Handy, and W. A. Lester Jr}}, - Journal = {Mol. Phys.}, - Pages = {3069}, - Volume = {104}, - Year = {2006}} - -@article{GamCatGra-PRC-09, - Author = {D. Gambacurta and F. Catara and M. Grasso}, - Journal = {Phys. Rev. C}, - Pages = {014303}, - Title = {{Self-consistent extension of random-phase approximation enlarged beyond particle-hole configurations}}, - Volume = {80}, - Year = {2009}} - -@article{GarAppGasBenFerPaqPraAssReiTouBarRenDavMalVerCafLooGinSce-JCTC-19, - Author = {Y. Garniron and T. Applencourt and K. Gasperich and A. Benali and A. Fert\'e and J. Paquier and B. Pradines and R. Assaraf and P. Reinhardt and J. Toulouse and P. Barbaresco and N. Renon and G. David and J.-P. Malrieu and M. V\'eril and M. Caffarel and P.-F. Loos and E. Giner and A. Scemama}, - Doi = {10.1021/acs.jctc.9b00176}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3591}, - Title = {Quantum Package 2.0: An open-source determinant-driven suite of programs}, - Volume = {15}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1021/acs.jctc.9b00176}} - -@misc{GarAppGasBenFerPaqPraAssReiTouBarRenDavMalVerCafLooGinSce-JJJ-XX, - Author = {Y. Garniron and T. Applencourt and K. Gasperich and A. Benali and A. Fert\'e and J. Paquier and B. Pradines and R. Assaraf and P. Reinhardt and J. Toulouse and P. Barbaresco and N. Renon and G. David and J.-P. Malrieu and M. V\'eril and M. Caffarel and P.-F. Loos and E. Giner and A. Scemama}, - Note = {Quantum Package 2.0: An open-source determinant-driven suite of programs, {\it submitted to J. Chem. Theory Comput.}, \href{https://arxiv.org/abs/1902.08154}{arXiv:1902.08154}}} - -@article{GarBulHenScu-JCP-15, - Author = {Alejandro J. Garza and Ireneusz W. Bulik and Thomas M. Henderson and Gustavo E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {044109}, - Volume = {142}, - Year = {2015}} - -@article{GarBulHenScu-PCCP-15, - Author = {A. J. Garza and I. W. Bulik and T. M. Henderson and G. E. Scuseria}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {22412}, - Volume = {17}, - Year = {2015}} - -@article{GarBulSouSunPerScu-MP-16, - Author = {{A. J. Garza, I. W. Bulik, A. G. Sousa Alencar, J. Sun, J. P. Perdew, and G. E. Scuseria}}, - Journal = {Mol. Phys.}, - Pages = {997}, - Volume = {114}, - Year = {2016}} - -@article{GarJimScu-JCP-13, - Author = {Alejandro J. Garza and Carlos A. Jim\'enez-Hoyos and Gustavo E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {134102}, - Volume = {138}, - Year = {2013}} - -@misc{Gaussian-PROG-03, - Author = {M. J. Frisch and G. W. Trucks and H. B. Schlegel and G. E. Scuseria and M. A. Robb and J. R. Cheeseman and Montgomery, Jr., J. A. and T. Vreven and K. N. Kudin and J. C. Burant and J. M. Millam and S. S. Iyengar and J. Tomasi and V. Barone and B. Mennucci and M. Cossi and G. Scalmani and N. Rega and G. A. Petersson and H. Nakatsuji and M. Hada and M. Ehara and K. Toyota and R. Fukuda and J. Hasegawa and M. Ishida and T. Nakajima and Y. Honda and O. Kitao and H. Nakai and M. Klene and X. Li and J. E. Knox and H. P. Hratchian and J. B. Cross and V. Bakken and C. Adamo and J. Jaramillo and R. Gomperts and R. E. Stratmann and O. Yazyev and A. J. Austin and R. Cammi and C. Pomelli and J. W. Ochterski and P. Y. Ayala and K. Morokuma and G. A. Voth and P. Salvador and J. J. Dannenberg and V. G. Zakrzewski and S. Dapprich and A. D. Daniels and M. C. Strain and O. Farkas and D. K. Malick and A. D. Rabuck and K. Raghavachari and J. B. Foresman and J. V. Ortiz and Q. Cui and A. G. Baboul and S. Clifford and J. Cioslowski and B. B. Stefanov and G. Liu and A. Liashenko and P. Piskorz and I. Komaromi and R. L. Martin and D. J. Fox and T. Keith and M. A. Al-Laham and C. Y. Peng and A. Nanayakkara and M. Challacombe and P. M. W. Gill and B. Johnson and W. Chen and M. W. Wong and C. Gonzalez and J. A. Pople}, - Note = {\uppercase{G}aussian, Inc., Wallingford, CT, 2004}, - Title = {Gaussian 03, \uppercase{R}evision \uppercase{C}.02}} - -@misc{Gaussian-PROG-09, - Author = {M. J. Frisch and G. W. Trucks and H. B. Schlegel and G. E. Scuseria and M. A. Robb and J. R. Cheeseman and G. Scalmani and V. Barone and B. Mennucci and G. A. Petersson and H. Nakatsuji and M. Caricato and X. Li and H. P. Hratchian and A. F. Izmaylov and J. Bloino and G. Zheng and J. L. Sonnenberg and M. Hada and M. Ehara and K. Toyota and R. Fukuda and J. Hasegawa and M. Ishida and T. Nakajima and Y. Honda and O. Kitao and H. Nakai and T. Vreven and Montgomery, {Jr.}, J. A. and J. E. Peralta and F. Ogliaro and M. Bearpark and J. J. Heyd and E. Brothers and K. N. Kudin and V. N. Staroverov and R. Kobayashi and J. Normand and K. Raghavachari and A. Rendell and J. C. Burant and S. S. Iyengar and J. Tomasi and M. Cossi and N. Rega and J. M. Millam and M. Klene and J. E. Knox and J. B. Cross and V. Bakken and C. Adamo and J. Jaramillo and R. Gomperts and R. E. Stratmann and O. Yazyev and A. J. Austin and R. Cammi and C. Pomelli and J. W. Ochterski and R. L. Martin and K. Morokuma and V. G. Zakrzewski and G. A. Voth and P. Salvador and J. J. Dannenberg and S. Dapprich and A. D. Daniels and {\"O}. Farkas and J. B. Foresman and J. V. Ortiz and J. Cioslowski and D. J. Fox}, - Note = {\uppercase{G}aussian Inc. Wallingford CT 2009}, - Title = {Gaussian~09 {R}evision {A}.1}} - -@article{GelBru-PR-57, - Author = {M. Gell-Mann and K. A. Brueckner}, - Journal = {Phys. Rev.}, - Pages = {364}, - Title = {Correlation Energy of an Electron Gas at High Density}, - Volume = {{106}}, - Year = {1957}} - -@article{GelTay-CJP-70a, - Author = {D. J. W. Geldart and R. Taylor}, - Journal = {Can. J. Phys.}, - Pages = {167}, - Volume = {{48}}, - Year = {1970}} - -@article{GelTay-CJP-70, - Author = {D. J. W. Geldart and R. Taylor}, - Journal = {Can. J. Phys.}, - Pages = {155}, - Volume = {{48}}, - Year = {1970}} - -@article{GelVos-CJP-66, - Author = {D. J. W. Geldart and S. H. Vosko}, - Journal = {Can. J. Phys.}, - Pages = {2137}, - Volume = {{44}}, - Year = {1966}} - -@article{GerAng-CPL-05a, - Author = {I. C. Gerber and J. G. \'Angy\'an}, - Journal = {Chem. Phys. Lett.}, - Pages = {100}, - Volume = {415}, - Year = {2005}} - -@article{GerAng-CPL-05b, - Author = {I. C. Gerber and J. G. \'Angy\'an}, - Journal = {Chem. Phys. Lett.}, - Pages = {370}, - Title = {Potential curves for alkaline-earth dimers by density functional theory with long-range correlation corrections}, - Volume = {416}, - Year = {2005}} - -@article{GerAng-CPL-05, - Author = {I. Gerber and J. G. \'Angy\'an}, - Journal = {Chem. Phys. Lett.}, - Pages = {100}, - Volume = {415}, - Year = {2005}} - -@article{GerAng-JCP-07, - Author = {I. C. Gerber and J. G. \'Angy\'an}, - Journal = {J. Chem. Phys.}, - Pages = {044103}, - Volume = {126}, - Year = {2007}} - -@article{GerAngMarKre-JCP-07, - Author = {I. C. Gerber and J. G. \'Angy\'an and M. Marsman and G. Kresse}, - Journal = {J. Chem. Phys.}, - Pages = {054101}, - Volume = {127}, - Year = {2007}} - -@misc{GerAngSavTou-JJJ-XX, - Author = {I. Gerber and J. G. \'Angy\'an and A. Savin and J. Toulouse}, - Note = {in preparation}, - Volume = {{}}} - -@article{ghosh:2976, - Author = {Swapan K. Ghosh and Max Berkowitz}, - Journal = {The Journal of Chemical Physics}, - Keywords = {HYDRODYNAMICS; QUANTUM MECHANICS; FUNCTIONALS; CORRELATION FUNCTIONS; ELECTRONIC STRUCTURE; ELECTRON CORRELATION}, - Number = {6}, - Pages = {2976-2983}, - Publisher = {AIP}, - Title = {A classical fluid-like approach to the density-functional formalism of many-electron systems}, - Url = {http://link.aip.org/link/?JCP/83/2976/1}, - Volume = {83}, - Year = {1985}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/83/2976/1}} - -@article{GhoPar-JCP-85, - Author = {Swapan K. Ghosh and Robert G. Parr}, - Journal = {The Journal of Chemical Physics}, - Keywords = {ELECTRONIC STRUCTURE; FUNCTIONALS; DENSITY MATRIX; ATOMS; WAVE FUNCTIONS}, - Number = {7}, - Pages = {3307-3315}, - Publisher = {AIP}, - Title = {Density-determined orthonormal orbital approach to atomic energy functionals[sup a)]}, - Url = {http://link.aip.org/link/?JCP/82/3307/1}, - Volume = {82}, - Year = {1985}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/82/3307/1}} - -@article{GidPapGro-PRL-02, - Author = {N. I. Gidopoulos and P. G. Papaconstantinou and E. K. U. Gross}, - Journal = {Phys. Rev. Lett.}, - Pages = {033003}, - Volume = {88}, - Year = {2002}} - -@article{GieBae-CPL-08, - Author = {K. J. H. Giesbertz and E. J. Baerends}, - Journal = {Chem. Phys. Lett.}, - Pages = {338}, - Volume = {461}, - Year = {2008}} - -@article{GieBaeGri-PRL-08, - Author = {K. J. H. Giesbertz and E. J. Baerends and O. V. Gritsenko}, - Journal = {Phys. Rev. Lett.}, - Pages = {033004}, - Volume = {101}, - Year = {2008}} - -@article{GieLee-JCP-13b, - Author = {{K. J. H. Giesbertz and R. van Leeuwen}}, - Journal = {J. Chem. Phys.}, - Pages = {104110}, - Volume = {139}, - Year = {2013}} - -@article{GieLee-JCP-13, - Author = {{K. J. H. Giesbertz and R. van Leeuwen}}, - Journal = {J. Chem. Phys.}, - Pages = {104109}, - Volume = {139}, - Year = {2013}} - -@article{GiePerGriBae-JCP-09, - Author = {K. J. H. Giesbertz and K. Pernal and O. V. Gritsenko and E. J. Baerends}, - Journal = {J. Chem. Phys.}, - Pages = {114104}, - Volume = {130}, - Year = {2009}} - -@article{GilAda-CPL-96, - Author = {P. M. W Gill and R. D. Adamson}, - Journal = {Chem. Phys. Lett.}, - Pages = {105}, - Volume = {{261}}, - Year = {1996}} - -@article{GilAdaPop-MP-96, - Author = {P. M. W. Gill and R. D. Adamson and J. A. Pople}, - Journal = {Mol. Phys.}, - Pages = {1005}, - Volume = {88}, - Year = {1996}} - -@article{GilBesGil-JPCA-08, - Author = {A. T. B. Gilbert and N. A. Besley and P. M. W. Gill}, - Journal = {J. Phys. Chem. A}, - Pages = {13164}, - Volume = {112}, - Year = {2008}} - -@article{GilCriOneBes-PCCP-06, - Author = {P. M. W. Gill and D. L. Crittenden and D. P. O'Neill and N. A. Besley}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {15}, - Volume = {8}, - Year = {2006}} - -@article{GilLeeNarAda-JMS-00, - Author = {P. M. W. Gill and A.M. Lee and N. Nair and R.D. Adamson}, - Journal = {J. Mol. Struct. (Theochem)}, - Pages = {303}, - Volume = {506}, - Year = {2000}} - -@article{GilOneBes-TCA-03, - Author = {P. M. W. Gill and Darragh O'Neill and N. A. Besley}, - Journal = {Theor. Chim. Acc.}, - Pages = {241}, - Volume = {109}, - Year = {2003}} - -@article{GilOne-JCP-05, - Author = {P. M. W. Gill and D. P. O'Neill}, - Journal = {J. Chem. Phys.}, - Pages = {094110}, - Volume = {122}, - Year = {2005}} - -@book{GilRicSpi-BOOK-96, - Address = {London}, - Author = {W. R. Gilks and S. Richardson and D. J. Spiegelhalter}, - Publisher = {Chapman \& Hall}, - Title = {{Markov Chain Monte Carlo in Practice}}, - Year = {1996}} - -@article{Gil-RMP-63, - Author = {T. L. Gilbert}, - Journal = {Rev. Mod. Phys.}, - Pages = {491}, - Title = {Interpretation of the Rapid Convergence of Correlation Wave Functions}, - Volume = {{35}}, - Year = {1963}} - -@article{GinAssTou-MP-16, - Author = {E. Giner and R. Assaraf and J. Toulouse}, - Doi = {http://dx.doi.org/./..}, - Journal = {Mol. Phys.}, - Pages = {910-920}, - Title = {Quantum Monte Carlo with reoptimized perturbatively selected configuration-interaction wave functions}, - Volume = {114}, - Year = {2016}, - Bdsk-Url-1 = {http://dx.doi.org/%EF%9B%9C%EF%98%B9.%EF%9B%9C%EF%98%B9%EF%99%80%EF%98%B9/%EF%98%B9%EF%98%B9%EF%98%BA%EF%98%BE%EF%99%80%EF%99%81%EF%98%BF%EF%98%BE.%EF%98%BA%EF%98%B9%EF%9B%9C%EF%98%BE.%EF%9B%9C%EF%9B%9C%EF%98%BC%EF%99%81%EF%98%BE%EF%98%BB%EF%98%B9}} - -@article{GinPraFerAssSavTou-JCP-18, - Author = {Emmanuel Giner and Barth\'elemy Pradines and Anthony Fert\'e and Roland Assaraf and Andreas Savin and Julien Toulouse}, - Journal = {J. Chem. Phys.}, - Pages = {194301}, - Title = {Curing basis-set convergence of wave-function theory using density-functional theory: A systematically improvable approach}, - Volume = {149}, - Year = {2018}} - -@article{GinSceCaf-CJC-13, - Author = {E. Giner and A. Scemama and M. Caffarel}, - Journal = {Can. J. Chem.}, - Pages = {879}, - Title = {Using perturbatively selected configuration interaction in quantum Monte Carlo calculations}, - Volume = {91}, - Year = {2013}} - -@article{GinSceTouLoo-JCP-19, - Author = {E. Giner and A. Scemama and J. Toulouse and P.-F. Loos}, - Doi = {10.1063/1.5122976}, - Journal = {J. Chem. Phys.}, - Pages = {144118}, - Title = {Chemically accurate excitation energies with small basis sets}, - Volume = {151}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5122976}} - -@article{GisGroRosSniBae-JPCA-99, - Author = {S. J. A. van Gisbergen and J. A. Groeneveld and A. Rosa and J. G. Snijders and E. J. Baerends}, - Journal = {J. Phys. Chem. A}, - Pages = {6835}, - Volume = {103}, - Year = {1999}} - -@article{GisSniBae-CPC-99, - Author = {{S. J. A. van Gisbergen, J. G. Snijders, and E. J. Baerends}}, - Journal = {Comp. Phys. Comm.}, - Pages = {119}, - Volume = {118}, - Year = {1999}} - -@article{GisSniBae-JCP-95, - Author = {{S. J. A. van Gisbergen, J. G. Snijders, and E. J. Baerends}}, - Journal = {J. Chem. Phys.}, - Pages = {9347}, - Volume = {103}, - Year = {1995}} - -@article{GlePeaToz-JCTC-13, - Author = {J. D. Gledhill and M. J. G. Peach and D. J. Tozer}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4414}, - Volume = {9}, - Year = {2013}} - -@article{GluLev-JCP-07, - Author = {V. N. Glushkov and M. Levy}, - Journal = {J. Chem. Phys.}, - Pages = {174106}, - Volume = {126}, - Year = {2007}} - -@article{GodDunHunJef-ACR-73, - Author = {{W. A. Goddard III, T. H. Dunning Jr., W. J. Hunt and P. J. Hay}}, - Journal = {Acc. Chem. Res.}, - Pages = {398}, - Volume = {6}, - Year = {1973}} - -@article{GodOrl-JCP-99, - Author = {John D. Goddard and Galina Orlova}, - Journal = {J. Chem. Phys.}, - Number = {17}, - Pages = {7705}, - Title = {Density functional theory with fractionally occupied frontier orbitals and the instabilities of the Kohn--Sham solutions for defining diradical transition states: Ring-opening reactions}, - Volume = {111}, - Year = {1999}} - -@article{God-SJMA-09, - Author = {B. D. Goddard}, - Journal = {Siam J. Math. Anal.}, - Pages = {77}, - Volume = {41}, - Year = {2009}} - -@article{GoeGri-JCTC-11, - Author = {L. Goerigk and S. Grimme}, - Journal = {J. Chem. Theory Comput.}, - Pages = {291}, - Volume = {7}, - Year = {2011}} - -@article{GoeGri-WIRE-14, - Author = {L. Goerigk and S. Grimme}, - Journal = {WIREs Comput. Mol. Sci.}, - Pages = {576}, - Volume = {4}, - Year = {2014}} - -@incollection{GoeUmr-INC-00, - Address = {Dordrecht/New York}, - Author = {S. Goedecker and C. J. Umrigar}, - Booktitle = {Many-Electron Densities and Reduced Density Matrices}, - Editor = {J. Cioslowski}, - Pages = {165-181}, - Publisher = {Kluwer Academic}, - Year = {2000}} - -@article{GoeUmr-PRL-98, - Author = {S. Goedecker and C. J. Umrigar}, - Journal = {Phys. Rev. Lett.}, - Pages = {866}, - Volume = {81}, - Year = {1998}} - -@article{GolErnMoeSto-JCP-09, - Author = {E. Goll and M. Ernst and F. Moegle-Hofacker and H. Stoll}, - Journal = {J. Chem. Phys.}, - Pages = {234112}, - Volume = {130}, - Year = {2009}} - -@article{GolLeiManMitWerSto-PCCP-08, - Author = {E. Goll and T. Leininger and F. R. Manby and A. Mitrushchenkov and H.-J. Werner and H. Stoll}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {3353}, - Title = {Local and density fitting approximations within the short-range/long-range hybrid scheme: application to large non-bonded complexes}, - Volume = {10}, - Year = {2008}} - -@article{GolSho-JPB-78, - Author = {A. Goldberg and B. W. Shore}, - Journal = {J. Phys. B}, - Pages = {3339}, - Volume = {11}, - Year = {1978}} - -@article{GolStoThiSch-PRA-07, - Author = {E. Goll and H. Stoll and C. Thierfelder and P. Schwerdtfeger}, - Journal = {Phys. Rev. A}, - Pages = {032507}, - Title = {Improved dipole moments by combining short-range gradient-corrected density-functional theory with long-range wave-function methods}, - Volume = {76}, - Year = {2007}} - -@article{GolWerSto-CP-08, - Author = {E. Goll and H.-J. Werner and H. Stoll}, - Journal = {Chem. Phys.}, - Pages = {257}, - Title = {Short-range density functionals in combination with local long-range ab initio methods: Application to non-bonded complexes}, - Volume = {346}, - Year = {2008}} - -@article{GolWerStoLeiGorSav-CP-06, - Author = {E. Goll and H.-J. Werner and H. Stoll and T. Leininger and P. Gori-Giorgi and A. Savin}, - Journal = {Chem. Phys.}, - Pages = {276}, - Volume = {329}, - Year = {2006}} - -@article{GolWerSto-PCCP-05, - Author = {Erich Goll and Hans-Joachim Werner and Hermann Stoll}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {3917}, - Title = {A short-range gradient-corrected density functional in long-range coupled-cluster calculations for rare gas dimers}, - Volume = {7}, - Year = {2005}} - -@article{GonHanKalHea-JCP-05, - Author = {V. Goncharov and J. Han and L. A. Kaledin and M. C. Heaven}, - Journal = {J. Chem. Phys.}, - Pages = {204311}, - Volume = {122}, - Year = {2005}} - -@article{GonSch-PRL-99, - Author = {X. Gonze and M. Scheffler}, - Journal = {Phys. Rev. Lett.}, - Pages = {4416}, - Volume = {82}, - Year = {1999}} - -@article{GorHeiLev-JMS-00, - Author = {A. G\"orling and H. H. Heinze and M. Levy}, - Journal = {J. Mol. Struct. (Theochem)}, - Pages = {271}, - Volume = {501}, - Year = {2000}} - -@article{GorHelScuSilTou-MP-16, - Author = {Paola Gori-Giorgi and Trygve Helgaker and Gustavo Scuseria and Bernard Silvi and Julien Toulouse}, - Doi = {http://dx.doi.org/./..}, - Journal = {Molecular Physics}, - Pages = {909}, - Title = {Foreword for special issue of Molecular Physics in honour of Andreas Savin}, - Volume = {114}, - Year = {2016}, - Bdsk-Url-1 = {http://dx.doi.org/%EF%9B%9C%EF%98%B9.%EF%9B%9C%EF%98%B9%EF%99%80%EF%98%B9/%EF%98%B9%EF%98%B9%EF%98%BA%EF%98%BE%EF%99%80%EF%99%81%EF%98%BF%EF%98%BE.%EF%98%BA%EF%98%B9%EF%9B%9C%EF%98%BE.%EF%9B%9C%EF%9B%9C%EF%98%BE%EF%98%B9%EF%98%BE%EF%98%BC%EF%98%BF}} - -@article{Gor-IJQC-98, - Author = {A. G\"orling}, - Journal = {Int. J. Quantum Chem.}, - Pages = {265}, - Volume = {69}, - Year = {1998}} - -@article{GorInd-PRA-88, - Author = {O. Gorceix and P. Indelicato}, - Journal = {Phys. Rev. A}, - Pages = {1087}, - Volume = {37}, - Year = {1988}} - -@article{Gor-JCP-05, - Author = {A. G\"orling}, - Journal = {J. Chem. Phys.}, - Pages = {062203}, - Volume = {123}, - Year = {2005}} - -@article{GorLev-IJQC-95, - Author = {A. G\"orling and M. Levy}, - Issue = {S29}, - Journal = {Int. J. Quantum Chem. Symp.}, - Pages = {93}, - Volume = {56}, - Year = {1995}} - -@article{GorLev-PRA-94, - Author = {A. G\"{o}rling and M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {196}, - Volume = {50}, - Year = {1994}} - -@article{GorLev-PRA-95, - Author = {A. G\"{o}rling and M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {4493}, - Volume = {52}, - Year = {1995}} - -@article{GorLev-PRB-93, - Author = {A. G\"{o}rling and M. Levy}, - Journal = {Phys. Rev. B}, - Pages = {13105}, - Volume = {47}, - Year = {1993}} - -@article{GorPer-PRB-01, - Author = {P. Gori-Giorgi and J. P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {155102}, - Volume = {{64}}, - Year = {2001}} - -@article{Gor-PRA-96, - Author = {A. G\"{o}rling}, - Journal = {Phys. Rev. A}, - Pages = {3912}, - Volume = {54}, - Year = {1996}} - -@article{Gor-PRA-98, - Author = {A. G\"{o}rling}, - Journal = {Phys. Rev. A}, - Pages = {3433}, - Volume = {57}, - Year = {1998}} - -@article{Gor-PRA-99, - Author = {A. G\"{o}rling}, - Journal = {Phys. Rev. A}, - Pages = {3359}, - Volume = {59}, - Year = {1999}} - -@misc{Gor-PRIV-XX, - Author = {P. Gori-Giorgi}, - Title = {private communication}} - -@article{Gor-PRL-00, - Author = {A. G\"orling}, - Journal = {Phys. Rev. Lett.}, - Pages = {4229}, - Volume = {85}, - Year = {2000}} - -@article{Gor-PRL-99, - Author = {A. G\"orling}, - Journal = {Phys. Rev. Lett.}, - Pages = {5459}, - Volume = {83}, - Year = {1999}} - -@article{GorSacBac-PRB-00, - Author = {P. Gori-Giorgi and F. Sacchetti and G. B. Bachelet}, - Journal = {Phys. Rev. B}, - Pages = {7353}, - Volume = {{61}}, - Year = {2000}} - -@article{GorSav-IJQC-09a, - Author = {P. Gori-Giorgi and A; Savin}, - Journal = {Int. J. Quantum Chem.}, - Pages = {1950}, - Volume = {109}, - Year = {2009}} - -@article{GorSav-IJQC-09, - Author = {P. Gori-Giorgi and A; Savin}, - Journal = {Int. J. Quantum Chem.}, - Pages = {2410}, - Volume = {109}, - Year = {2009}} - -@misc{GorSav-JJJ-XX, - Author = {P. Gori-Giorgi and A. Savin}, - Note = {cond-mat/611324}} - -@article{GorSav-JPCS-08, - Author = {P. Gori-Giorgi and A. Savin}, - Journal = {J. Phys.: Conf. Ser.}, - Pages = {012017}, - Volume = {117}, - Year = {2008}} - -@article{GorSav-PM-06, - Author = {P. Gori-Giorgi and A. Savin}, - Journal = {Phil. Mag.}, - Pages = {2643}, - Volume = {86}, - Year = {2006}} - -@article{GorSav-PRA-05, - Author = {P. Gori-Giorgi and A. Savin}, - Journal = {Phys. Rev. A}, - Pages = {032513}, - Volume = {71}, - Year = {2005}} - -@article{GorSav-PRA-06, - Author = {P. Gori-Giorgi and A. Savin}, - Journal = {Phys. Rev. A}, - Pages = {032506}, - Volume = {73}, - Year = {2006}} - -@article{GorSeiSav-PCCP-08, - Author = {P. Gori-Giorgi and M. Seidl and A. Savin}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {3440}, - Volume = {10}, - Year = {2008}} - -@article{GorZie-PRB-02, - Author = {P. Gori-Giorgi and P. Ziesche}, - Journal = {Phys. Rev. B}, - Pages = {235116}, - Volume = {{66}}, - Year = {2002}} - -@article{GouDob-JCP-13, - Author = {T. Gould and J. F. Dobson}, - Journal = {J. Chem. Phys.}, - Pages = {014103}, - Volume = {138}, - Year = {2013}} - -@article{GouDob-PRB-11, - Author = {T. Gould and J. F. Dobson}, - Journal = {Phys. Rev. B}, - Pages = {241108}, - Volume = {84}, - Year = {2011}} - -@article{Gou-JCP-12, - Author = {T. Gould}, - Journal = {J. Chem. Phys.}, - Pages = {111101}, - Volume = {137}, - Year = {2012}} - -@article{GouMalSal-TCA-95, - Author = {A. Goursot and J. P. Malrieu and D. R. Salahub}, - Journal = {Theor. Chim. Acta}, - Pages = {225}, - Volume = {91}, - Year = {1995}} - -@article{GouPitTouKraKro-PCCP-19, - Author = {T. Gould and S. Pittalis and J. Toulouse and E. Kraisler and L. Kronik}, - Doi = {10.1039/c9cp03633d}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {19805}, - Title = {Asymptotic behavior of the Hartree-exchange and correlation potentials in ensemble density functional theory}, - Volume = {21}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1039/c9cp03633d}} - -@article{GouTouAngDob-JCTC-17, - Author = {Tim Gould and Julien Toulouse and J\'anos G. \'Angy\'an and John F. Dobson}, - Doi = {10.1021/acs.jctc.7b00996}, - Journal = {J. Chem. Theory Comput.}, - Pages = {5829}, - Title = {Casimir--Polder Size Consistency: A Constraint Violated by Some Dispersion Theories}, - Volume = {13}, - Year = {2017}, - Bdsk-Url-1 = {https://doi.org/10.1021/acs.jctc.7b00996}} - -@article{GouTou-PRA-14, - Author = {T. Gould and J. Toulouse}, - Doi = {http://dx.doi.org/10.1103/PhysRevA.90.050502}, - Journal = {Phys. Rev. A}, - Pages = {050502(R)}, - Title = {{Kohn-Sham potentials in exact density-functional theory at noninteger electron numbers}}, - Volume = {90}, - Year = {2014}, - Bdsk-Url-1 = {http://dx.doi.org/10.1103/PhysRevA.90.050502}} - -@article{GraCre-CPL-00, - Author = {J. Grafenstein and D. Cremer}, - Journal = {Chem. Phys. Lett.}, - Pages = {569}, - Volume = {{316}}, - Year = {2000}} - -@article{GraCre-MP-05, - Author = {J. Gr\"afenstein and D. Cremer}, - Journal = {Mol. Phys.}, - Pages = {279}, - Title = {{Development of a CAS-DFT method covering non-dynamical and dynamical electron correlation in a balanced way}}, - Volume = {103}, - Year = {2005}} - -@article{GraCre-PCCP-00, - Author = {J. Gr\"afenstein and Dieter Cremer}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {2091}, - Volume = {2}, - Year = {2000}} - -@article{GraFabTeaSmiBukDel-JCP-14, - Author = {{I. Grabowski, E. Fabiano, A. M. Teale, S. \'Smiga, A. Buksztel, and F. Della Sala}}, - Journal = {J. Chem. Phys.}, - Pages = {024113}, - Volume = {141}, - Year = {2014}} - -@article{GraGro-CPL-95, - Author = {T. Grabo and E. K. U. Gross}, - Journal = {Chem. Phys. Lett.}, - Pages = {141}, - Volume = {240}, - Year = {1995}} - -@article{GraHirIvaBar-JCP-02, - Author = {I. Grabowski and S. Hirata and S. Ivanov and R. J. Bartlett}, - Journal = {J. Chem. Phys.}, - Pages = {4415}, - Volume = {116}, - Year = {2002}} - -@article{GraKraCre-JCP-04, - Author = {J. Gr\"afenstein and E. Kraka and D. Cremer}, - Journal = {J. Chem. Phys.}, - Pages = {524}, - Volume = {120}, - Year = {2004}} - -@incollection{GraKreKurGro-INC-00, - Address = {Tokyo}, - Author = {T. Grabo and T. Kreibich and S. Kurth and E. K. U. Gross}, - Booktitle = {Strong Coulomb Correlation in Electronic Structure: Beyond the Local Density Approximation}, - Editor = {V. Anisimov}, - Publisher = {Gordon \& Breach}, - Title = {Orbital functionals in density functional theory: the optimized effective potential method}, - Year = {2000}} - -@article{GraMenGoeGriRad-JPCA-09, - Author = {D. C. Graham and A. S. Menon and L. Goerigk and S. Grimme and L. Radom}, - Journal = {J. Phys. Chem. A}, - Pages = {9861}, - Volume = {113}, - Year = {2009}} - -@article{GraTeaFabSmiBukDel-MP-14, - Author = {{I. Grabowski, A. M. Teale, E. Fabiano, S. \'Smiga, A. Buksztel, and F. Della Sala}}, - Journal = {Mol. Phys.}, - Pages = {700}, - Volume = {112}, - Year = {2014}} - -@article{GraTeaSmiBar-JCP-11, - Author = {I. Grabowski and A. M. Teale and S. \'Smiga and R. J. Bartlett}, - Journal = {J. Chem. Phys.}, - Pages = {114111}, - Volume = {135}, - Year = {2011}} - -@article{GreCha-CPL-71, - Author = {F. Grein and T. C. Chang}, - Journal = {Chem. Phys. Lett.}, - Pages = {44}, - Volume = {12}, - Year = {1971}} - -@article{GreHoPabKamMazSan-PRA-10, - Author = {L. Greenman and P. J. Ho and S. Pabst and E. Kamarchik and D. A. Mazziotti and R. Santra}, - Journal = {Phys. Rev. A}, - Pages = {023406}, - Volume = {82}, - Year = {2010}} - -@article{GreRok-JCP-87, - Author = {L. Greengard and V. Rokhlin}, - Journal = {J. Comput. Phys.}, - Pages = {325}, - Volume = {{73}}, - Year = {1987}} - -@article{GriAntEhrKri-JCP-10, - Author = {S. Grimme and J. Antony and S. Ehrlich and H. Krieg}, - Journal = {J. Chem. Phys.}, - Pages = {154104}, - Title = {{A consistent and accurate ab initio parametrization of density functional dispersion correction (DFT-D) for the 94 elements H-Pu}}, - Volume = {132}, - Year = {2010}} - -@article{Gri-CPL-96, - Author = {S. Grimme}, - Journal = {Chem. Phys. Lett.}, - Pages = {128}, - Volume = {259}, - Year = {1996}} - -@article{GriGisGorBae-JCP-00, - Author = {{O. V. Gritsenko, S. J. A. van Gisbergen, A. G\"orling, and E. J. Baerends}}, - Journal = {J. Chem. Phys.}, - Pages = {8478}, - Volume = {113}, - Year = {2000}} - -@article{Gri-JCC-04, - Author = {S. Grimme}, - Journal = {J. Comput. Chem.}, - Pages = {1463}, - Volume = {25}, - Year = {2004}} - -@article{Gri-JCP-03, - Author = {S. Grimme}, - Journal = {J. Chem. Phys.}, - Pages = {9095}, - Volume = {118}, - Year = {2003}} - -@article{Gri-JCP-06, - Author = {S. Grimme}, - Journal = {J. Chem. Phys.}, - Pages = {034108}, - Title = {Semiempirical hybrid density functional with perturbative second-order correlation}, - Volume = {124}, - Year = {2006}} - -@article{GriLeeBae-IJQC-96, - Author = {{O. V. Gritsenko, R. van Leeuwen, and E. J. Baerends}}, - Journal = {Int. J. Quantum Chem.: Quantum Chem. Symp.}, - Pages = {1375}, - Volume = {30}, - Year = {1996}} - -@article{GriLud-JPB-02, - Author = {G. F. Gribakin and J. Ludlow}, - Journal = {J. Phys. B}, - Pages = {339}, - Volume = {35}, - Year = {2002}} - -@article{GriMeePer-CPL-19, - Author = {{O. V. Gritsenko, R. van Meer, and K. Pernal}}, - Journal = {Chem. Phys. Lett.}, - Pages = {227}, - Volume = {716}, - Year = {2019}} - -@article{GriMeePer-PRA-18, - Author = {{O. V. Gritsenko, R. van Meer, and K. Pernal}}, - Journal = {Phys. Rev. A}, - Pages = {062510}, - Volume = {98}, - Year = {2018}} - -@article{GriNee-JCP-07, - Author = {S. Grimme and F. Neese}, - Journal = {J. Chem. Phys.}, - Pages = {154116}, - Volume = {127}, - Year = {2007}} - -@article{GriPer-JCP-19, - Author = {O. V. Gritsenko and K. Pernal}, - Journal = {J. Chem. Phys.}, - Pages = {024111}, - Volume = {151}, - Year = {2019}} - -@article{GriSchBae-JCP-97, - Author = {O. V. Gritsenko and P. R. T. Schipper and E. J. Baerends}, - Journal = {J. Chem. Phys.}, - Pages = {5007}, - Volume = {107}, - Year = {1997}} - -@article{GriSie-JLMS-99, - Author = {M. Grisemer and H. Siedentop}, - Journal = {J. London Math. Soc.}, - Pages = {490}, - Volume = {60}, - Year = {1999}} - -@article{GriSte-PCCP-16, - Author = {S. Grimme and M. Steinmetz}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {20926}, - Volume = {18}, - Year = {2016}} - -@article{GriSto-JCP-69, - Author = {R. Grimm and R. G. Storer}, - Journal = {J. Comput. Phys.}, - Pages = {230}, - Volume = {4}, - Year = {1969}} - -@article{GriSto-JCP-71, - Author = {R. Grimm and R. G. Storer}, - Journal = {J. Comput. Phys.}, - Pages = {134}, - Title = {{Monte-Carlo solution of Schr\"odinger's equation}}, - Volume = {7}, - Year = {1971}} - -@article{GriWal-JCP-99, - Author = {S. Grimme and M. Waletzke}, - Journal = {J. Chem. Phys.}, - Number = {13}, - Pages = {5645}, - Title = {{A combination of Kohn-Sham density functional theory and multi-reference configuration interaction methods}}, - Volume = {111}, - Year = {1999}} - -@article{GroDre-ZPA-81, - Author = {E. K. U. Gross and R. M. Dreizler}, - Journal = {Z. Phys. A}, - Pages = {103}, - Volume = {302}, - Year = {1981}} - -@article{GroKoh-PRL-85, - Author = {E. K. U. Gross and W. Kohn}, - Journal = {Phys. Rev. Lett.}, - Pages = {2850}, - Volume = {55}, - Year = {1985}} - -@article{GroOliKoh-PRA-88, - Author = {E. K. U. Gross and L. N. Olivieria and W. Kohn}, - Journal = {Phys. Rev. A}, - Pages = {2809}, - Volume = {37}, - Year = {1988}} - -@article{GroRohMitLouCoh-PRL-01, - Author = {J. C. Grossman and M. Rohlfing and L. Mitas and S. G. Louie and M. L. Cohen}, - Journal = {Phys. Rev. Lett.}, - Pages = {472}, - Volume = {86}, - Year = {2001}} - -@book{GroRunHei-BOOK-91, - Address = {Bristol}, - Author = {E. K. U. Gross and E. Runge and O. Heinonen}, - Publisher = {Verlag Adam Hilger}, - Title = {Many-particle theory}, - Year = {1991}} - -@article{GruGriBae-JCP-02, - Author = {M. Gr\"uning and O. V. Gritsenko and E. J. Baerends}, - Journal = {J. Chem. Phys.}, - Pages = {6435}, - Volume = {116}, - Year = {2002}} - -@article{GruMarGon-CMS-11, - Author = {M. Gr\"uning and A. Marini and X. Gonze}, - Journal = {Comput. Mater. Sci.}, - Pages = {2148}, - Volume = {50}, - Year = {2011}} - -@article{GruMarGon-NL-09, - Author = {M. Gr\"uning and A. Marini and X. Gonze}, - Journal = {Nano Lett.}, - Pages = {2820}, - Volume = {9}, - Year = {2009}} - -@article{GruMarHarSchKre-JCP-09, - Author = {Andreas Gr\"uneis and Martijn Marsman and Judith Harl and Laurids Schimka and Georg Kresse}, - Journal = {J. Chem. Phys.}, - Pages = {154115}, - Volume = {131}, - Year = {2009}} - -@article{GucSanUmrJai-PRB-05, - Author = {A. D. G\"u\c{c}l\"u and Gun Sang Jeon and C. J. Umrigar and J. K. Jain}, - Journal = {Phys. Rev. B}, - Pages = {205327}, - Title = {Quantum Monte Carlo study of composite fermions in quantum dots: The effect of Landau-level mixing}, - Volume = {72}, - Year = {2005}} - -@article{GunJonLun-PRB-79, - Author = {O. Gunnarsson and M. Jonson and B. I. Lundqvist}, - Journal = {Phys. Rev. B}, - Pages = {3136}, - Volume = {{20}}, - Year = {1979}} - -@article{GunLun-PRB-76, - Author = {O. Gunnarsson and B. I. Lundqvist}, - Journal = {Phys. Rev. B}, - Pages = {4274}, - Title = {Exchange and correlation in atoms, molecules, and solids by the spin-density-functional formalism}, - Volume = {{13}}, - Year = {1976}} - -@article{GusHenSor-JCP-08, - Author = {G. E. Scuseria and T. M. Henderson and D. C. Sorensen}, - Journal = {J. Chem. Phys.}, - Pages = {231101}, - Volume = {129}, - Year = {2008}} - -@article{GusMalLinRoo-TCA-04, - Author = {Sergey Gusarov and P.-A. Malmqvist and Roland Lindh and B. O. Roos}, - Journal = {Theor. Chim. Acc.}, - Pages = {84}, - Volume = {112}, - Year = {2004}} - -@misc{GutSav-JJJ-XX, - Author = {C. Gutl\'e and A. Savin}, - Title = {in preparation}, - Volume = {{}}} - -@article{GutSav-PRA-07, - Author = {C. Gutl\'e and A. Savin}, - Journal = {Phys. Rev. A}, - Pages = {032519}, - Title = {Orbital spaces and density-functional theory}, - Volume = {75}, - Year = {2007}} - -@phdthesis{Gut-THESIS-03, - Author = {C. Gutl\'e}, - School = {Universit\'e Paris 7}, - Title = {Espaces orbitalaires et th\'eorie de la fonctionnelle de la densit\'e}, - Type = {Th\`ese de doctorat}, - Year = {2003}} - -@article{HahSchBec-PRB-05, - Author = {P. H. Hahn and W. G. Schmidt and F. Bechstedt}, - Journal = {Phys. Rev. B}, - Pages = {245425}, - Volume = {72}, - Year = {2005}} - -@article{HalHelJorKloKocOlsWil-CPL-98, - Author = {A. Halkier and T. Helgaker and P. J{\o}rgensen and W. Klopper and H. Koch and J. Olsen and A. K. Wilson}, - Journal = {Chem. Phys. Lett.}, - Pages = {243}, - Volume = {286}, - Year = {1998}} - -@article{HalHelJorKloOls-CPL-99, - Author = {A. Halkier and T. Helgaker and P. J{\o}rgensen and W. Klopper and J. Olsen}, - Journal = {Chem. Phys. Lett.}, - Pages = {437}, - Volume = {302}, - Year = {1999}} - -@book{HamLesRey-BOOK-94, - Address = {Singapore}, - Author = {B. L. Hammond and W. A. Lester, Jr. and P. J. Reynolds}, - Publisher = {World Scientific}, - Title = {Monte Carlo Methods in Ab Initio Quantum Chemistry}, - Year = {1994}} - -@article{HanBou-MP-79, - Author = {A. E. Hansen and T. D. Bouman}, - Journal = {Mol. Phys.}, - Pages = {1713}, - Volume = {37}, - Year = {1979}} - -@article{HarHanBou-JCP-89, - Author = {R. A. Harris and A. E. Hansen and T. D. Bouman}, - Journal = {J. Chem. Phys.}, - Pages = {5856}, - Volume = {91}, - Year = {1989}} - -@article{Har-IJQC-80, - Author = {J. E. Harriman}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {689}, - Volume = {17}, - Year = {1980}} - -@article{HarIri-IJQC-06, - Author = {J. A. W. Harkless and K. K. Irikura}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {2373}, - Volume = {106}, - Year = {2006}} - -@article{Har-JCP-69, - Author = {R. A. Harris}, - Journal = {J. Chem. Phys.}, - Pages = {3947}, - Volume = {50}, - Year = {1969}} - -@article{HarJon-JPF-74, - Author = {Harris, J. and Jones, R. O.}, - Journal = {J. Phys. F}, - Pages = {1170-1186}, - Title = {The surface energy of a bounded electron gas-solid}, - Volume = {4}, - Year = {1974}} - -@article{HarKre-PRB-08, - Author = {Judith Harl and Georg Kresse}, - Doi = {10.1103/PhysRevB.77.045136}, - Journal = {Phys. Rev. B.}, - Keywords = {ab initio calculations; argon; binding energy; density functional theory; dissociation energies; hydrogen; krypton; lattice constants; neon; nitrogen; oxygen; RPA calculations}, - Pages = {045136}, - Title = {Cohesive energy curves for noble gas solids calculated by adiabatic connection fluctuation-dissipation theory}, - Volume = {77}, - Year = {2008}, - Bdsk-Url-1 = {https://doi.org/10.1103/PhysRevB.77.045136}} - -@article{HarKre-PRL-09, - Author = {Judith Harl and Georg Kresse}, - Journal = {Phys. Rev. Lett.}, - Pages = {056401}, - Volume = {103}, - Year = {2009}} - -@article{Har-PRA-84, - Author = {J. Harris}, - Journal = {Phys. Rev. A}, - Pages = {1648}, - Volume = {{29}}, - Year = {1984}} - -@article{HarSchKre-PRB-10, - Author = {J. Harl and L. Schimka and G. Kresse}, - Journal = {Phys. Rev. B}, - Pages = {115126}, - Volume = {81}, - Year = {2010}} - -@article{Has-B-70, - Author = {W. K. Hastings}, - Journal = {Biometrika}, - Pages = {97}, - Title = {{Monte Carlo sampling methods using Markov chains and their applications}}, - Volume = {57}, - Year = {1970}} - -@article{HatSasNakPet-PTP-08, - Author = {Naomichi Hatano and Keita Sasada and Hiroaki Nakamura and Tomio Petrosky}, - Journal = {Prog. Theor. Phys.}, - Pages = {187}, - Title = {Some Properties of the Resonant State in Quantum Mechanics and Its Computation}, - Volume = {119}, - Year = {2008}} - -@article{HauKlo-JCP-12, - Author = {Haunschild, Robin and Klopper, Wim}, - Journal = {J. Chem. Phys.}, - Number = {16}, - Pages = {164102}, - Title = {New accurate reference energies for the G2/97 test set}, - Volume = {136}, - Year = {2012}} - -@article{HauKlo-TCA-12, - Author = {Haunschild, Robin and Klopper, Wim}, - Journal = {Theor. Chem. Acc.}, - Pages = {1112}, - Volume = {131}, - Year = {2012}} - -@article{HauKlo-TCA-12-err, - Author = {Haunschild, Robin and Klopper, Wim}, - Journal = {Theor. Chem. Acc.}, - Pages = {1306}, - Volume = {132}, - Year = {2013}} - -@article{HeaRicOumLee-CPL-94, - Author = {M. Head-Gordon and R. J. Rico and M. Oumi and T. J. Lee}, - Journal = {Chem. Phys. Lett.}, - Pages = {21}, - Volume = {219}, - Year = {1994}} - -@article{HedHeiKneFroJen-JCP-13, - Author = {E. D. Hedeg{\aa}rd and F. Heiden and S. Knecht and E. Fromager and H. J. Aa. Jensen}, - Journal = {J. Chem. Phys.}, - Pages = {184308}, - Volume = {139}, - Year = {2013}} - -@article{HedKneKieJenRei-JCP-15, - Author = {E. D. Hedeg{\aa}rd and S. Knecht and J. S. Kielberg and H. J. Aa. Jensen and M. Reiher}, - Journal = {J. Chem. Phys.}, - Pages = {224108}, - Volume = {142}, - Year = {2015}} - -@article{Hed-PR-65, - Author = {L. Hedin}, - Journal = {Phys. Rev.}, - Pages = {A 796}, - Volume = {{139}}, - Year = {1965}} - -@misc{HedTouJen-ARX-17, - Author = {E. D. Hedeg{\aa}rd and J. Toulouse and H. J. Aa. Jensen}, - Note = {arXiv:1711.03882}, - Title = {Multiconfigurational short-range density-functional theory for open-shell systems}} - -@article{HedTouJen-JCP-18, - Author = {E. D. Hedeg{\aa}rd and J. Toulouse and H. J. Aa. Jensen}, - Doi = {10.1063/1.5013306}, - Journal = {J. Chem. Phys.}, - Pages = {214103}, - Title = {Multiconfigurational short-range density-functional theory for open-shell systems}, - Volume = {148}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5013306}} - -@article{HehStePop-JCP-69, - Author = {W. J. Hehre and R. F. Stewart and J. A. Pople}, - Journal = {J. Chem. Phys.}, - Pages = {2657}, - Volume = {51}, - Year = {1969}} - -@article{HelBar-JCP-10, - Author = {Maria Hellgren and Ulf von Barth}, - Journal = {J. Chem. Phys.}, - Pages = {044101}, - Volume = {132}, - Year = {2010}} - -@article{HelBar-PRB-07, - Author = {Maria Hellgren and Ulf von Barth}, - Doi = {10.1103/PhysRevB.76.075107}, - Journal = {Phys. Rev. B}, - Keywords = {density functional theory; exchange interactions (electron); splines (mathematics); excitons; nanostructured materials}, - Pages = {075107}, - Title = {Correlation potential in density functional theory at the GWA level: Spherical atoms}, - Volume = {76}, - Year = {2007}, - Bdsk-Url-1 = {https://doi.org/10.1103/PhysRevB.76.075107}} - -@article{HelBar-PRB-08, - Author = {M. Hellgren and U. von Barth}, - Journal = {Phys. Rev. B}, - Pages = {115107}, - Volume = {78}, - Year = {2008}} - -@article{HelCarRohRenRubSchRin-PRB-15, - Author = {M. Hellgren and F. Caruso and D. R. Rohr and X. Ren and A. Rubio and M. Scheffler and P. Rinke}, - Journal = {Phys. Rev. B}, - Pages = {165110}, - Volume = {91}, - Year = {2015}} - -@article{HelColGir-PRB-18, - Author = {{M. Hellgren, N. Colonna, and S. de Gironcoli}}, - Journal = {Phys. Rev. B}, - Pages = {045117}, - Volume = {98}, - Year = {2018}} - -@article{HelCorJorKriOlsRuu-CR-12, - Author = {T. Helgaker and S. Coriani and P. J{\o}rgensen and K. Kristensen and J. Olsen and K. Ruud}, - Journal = {Chem. Rev.}, - Pages = {543}, - Title = {Recent Advances in Wave Function-Based Methods of Molecular-Property Calculations}, - Volume = {112}, - Year = {2012}} - -@article{HelGasIss-PRB-03, - Author = {Slimane Hellal and Jean-Georges Gasser and Arezki Issolah}, - Journal = {Phys. Rev. B}, - Keywords = {Monte Carlo methods; electron gas; dielectric function; exchange interactions (electron); electron correlations}, - Number = {9}, - Pages = {094204}, - Publisher = {APS}, - Title = {Static local-field correction from Monte Carlo studies of the homogeneous electron gas}, - Volume = {68}, - Year = {2003}} - -@book{HelJorOls-BOOK-02, - Address = {Chichester}, - Author = {T. Helgaker and Poul J{\o}rgensen and Jeppe Olsen}, - Publisher = {Wiley}, - Title = {Molecular Electronic-Structure Theory}, - Year = {2002}} - -@book{HelJorOls-BOOK-16, - Author = {T. Helgaker and Poul J{\o}rgensen and Jeppe Olsen}, - Publisher = {Wiley-Blackwell}, - Title = {Density--Functional Theory: A Convex Treatment}, - Year = {2016}} - -@article{HelKloKocNog-JCP-97, - Author = {T. Helgaker and W. Klopper and H. Koch and J. Noga}, - Journal = {J. Chem. Phys.}, - Pages = {9639}, - Volume = {106}, - Year = {1997}} - -@article{HelRohGro-JCP-12, - Author = {M. Hellgren and D. R. Rohr and E. K. U. Gross}, - Journal = {J. Chem. Phys.}, - Pages = {034106}, - Volume = {136}, - Year = {2012}} - -@article{Hel-TALK-XX, - Note = {{T. Helgaker, {\it Time-Independent Molecular Properties}, \url{http://folk.uio.no/helgaker/pres.html}}}} - -@article{HenBar-PRA-04, - Author = {Thomas M. Henderson and Rodney J. Bartlett}, - Eid = {022512}, - Journal = {Physical Review A (Atomic, Molecular, and Optical Physics)}, - Keywords = {quantum chemistry; electron correlations; wave functions}, - Number = {2}, - Numpages = {12}, - Pages = {022512}, - Publisher = {APS}, - Title = {Short-range corrections to the correlation hole}, - Url = {http://link.aps.org/abstract/PRA/v70/e022512}, - Volume = {70}, - Year = {2004}, - Bdsk-Url-1 = {http://link.aps.org/abstract/PRA/v70/e022512}} - -@article{HenIzmScuSav-JCP-07, - Author = {T. M. Henderson and A. F. Izmaylov and G. E. Scuseria and A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {221103}, - Volume = {127}, - Year = {2007}} - -@article{HenIzmScuSav-JCTC-08, - Author = {T. M. Henderson and A. F. Izmaylov and G. E. Scuseria and A. Savin}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1254}, - Volume = {4}, - Year = {2008}} - -@article{HenScu-MP-10, - Author = {T. M. Henderson and G. E. Scuseria}, - Journal = {Mol. Phys.}, - Pages = {2511}, - Volume = {108}, - Year = {2010}} - -@book{Her-BOOK-66, - Address = {New York}, - Author = {G. Herzberg}, - Publisher = {van Nostrand Reinhold}, - Title = {Molecular spectroscopy and molecular structure; Electronic spectra end electronic structure of polyatomic molecules, vol. III}, - Year = {1966}} - -@article{HerSch-PRL-08, - Author = {Andreas Hermann and Peter Schwerdtfeger}, - Journal = {Phys. Rev. Lett.}, - Pages = {183005}, - Volume = {101}, - Year = {2008}} - -@article{HesAng-TCA-18, - Author = {A. He{\ss}elmann and J. G. \'Angy\'an}, - Journal = {Theor. Chem. Acc.}, - Pages = {155}, - Volume = {137}, - Year = {2018}} - -@article{HesGor-MP-10, - Author = {A. He{\ss}elmann and A. G\"orling}, - Journal = {Mol. Phys.}, - Pages = {359}, - Volume = {108}, - Year = {2010}} - -@article{HesGor-PRL-11, - Author = {A. He{\ss}elmann and A. G\"orling}, - Journal = {Phys. Rev. Lett.}, - Pages = {093001}, - Volume = {106}, - Year = {2011}} - -@article{HesGotDelGor-JCP-07, - Author = {{A. He{\ss}elmann, A. W. G\"otz, F. Della Sala, and A. G\"orling}}, - Journal = {J. Chem. Phys.}, - Pages = {054102}, - Volume = {127}, - Year = {2007}} - -@article{HesJan-CPL-03, - Author = {A. He{\ss}elmann and G. Jansen}, - Journal = {Chem. Phys. Lett.}, - Pages = {778}, - Volume = {367}, - Year = {2003}} - -@article{HesJanSch-JCP-05, - Author = {A. He{\ss}elmann and G. Jansen and M. Sch\"utz}, - Journal = {J. Chem. Phys.}, - Pages = {014103}, - Volume = {122}, - Year = {2005}} - -@article{Hes-JCP-11, - Author = {A. He{\ss}elmann}, - Journal = {J. Chem. Phys.}, - Pages = {204107}, - Volume = {134}, - Year = {2011}} - -@article{Hes-PCCP-06, - Author = {A. He{\ss}elmann}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {563}, - Volume = {8}, - Year = {2006}} - -@article{HetSchStoWer-JCP-00, - Author = {G. Hetzer and M. Sch\"utz and H. Stoll and H.-J. Werner}, - Journal = {J. Chem. Phys.}, - Pages = {9443}, - Volume = {113}, - Year = {2000}} - -@article{HeyPerScuMar-JCP-05, - Author = {J. Heyd and J. E. Peralta and G. E. Scuseria and R. L. Martin}, - Journal = {J. Chem. Phys.}, - Pages = {174101}, - Volume = {{123}}, - Year = {2005}} - -@article{HeyScuErn-JCP-03, - Author = {J. Heyd and G. E. Scuseria and M. Ernzerhof}, - Journal = {J. Chem. Phys.}, - Pages = {8207}, - Volume = {{118}}, - Year = {2003}} - -@article{HeyScu-JCP-04b, - Author = {J. Heyd and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {1187}, - Volume = {{121}}, - Year = {2004}} - -@article{HeyScu-JCP-04, - Author = {J. Heyd and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {7274}, - Volume = {{120}}, - Year = {2004}} - -@article{HibHumByrLen-JCP-94, - Author = {{P. C. Hiberty S. Humbel, C. P. Byrman and J. H. van Lenthe}}, - Journal = {J. Chem. Phys.}, - Pages = {5969}, - Volume = {101}, - Year = {1994}} - -@article{HibHum-JCP-94, - Author = {P. C. Hiberty and S. Humbel and P. Archirel}, - Journal = {J. Chem. Phys.}, - Pages = {11697}, - Volume = {98}, - Year = {1994}} - -@article{HibSha-JComChem-07, - Author = {P. C. Hiberty and S. Shaik}, - Journal = {J. Comput. Chem.}, - Pages = {137}, - Volume = {28}, - Year = {2007}} - -@article{HibSha-TCA-02, - Author = {P. C. Hiberty and S. Shaik}, - Journal = {Theor. Chem. Acc.}, - Pages = {255}, - Volume = {108}, - Year = {2002}} - -@article{Hil-JCP-85, - Author = {R. N. Hill}, - Journal = {J. Chem. Phys.}, - Pages = {1173}, - Volume = {83}, - Year = {1985}} - -@article{HilPetKniWer-JCP-09, - Author = {J. G. Hill and K. A. Peterson and G. Knizia and H.-J. Werner}, - Journal = {J. Chem. Phys.}, - Pages = {194105}, - Volume = {131}, - Year = {2009}} - -@article{HilSucFei-PRA-78, - Author = {J. Hiller and J. Sucher and G. Feinberg}, - Journal = {Phys. Rev. A}, - Pages = {2399}, - Volume = {18}, - Year = {1978}} - -@article{HirHea-CPL-99, - Author = {So Hirata and Martin Head-Gordon}, - Journal = {Chem. Phys. Lett.}, - Pages = {291}, - Volume = {314}, - Year = {1999}} - -@article{HirIvaGraBarBurTal-JCP-01, - Author = {S. Hirata and S. Ivanov and I. Grabowski and R. J. Bartlett and K. Burke and J. D. Talman}, - Journal = {J. Chem. Phys.}, - Pages = {1635}, - Volume = {115}, - Year = {2001}} - -@article{HirIvaGraBar-JCP-02, - Author = {S. Hirata and S. Ivanov and I. Grabowski and R. J. Bartlett}, - Journal = {J. Chem. Phys.}, - Pages = {6468}, - Volume = {116}, - Year = {2002}} - -@article{Hir-JCP-05, - Author = {S. Hirata}, - Journal = {J. Chem. Phys.}, - Pages = {026101}, - Volume = {123}, - Year = {2005}} - -@article{HirNogSug-PRB-15, - Author = {D. Hirose and Y. Noguchi and O. Sugino}, - Journal = {Phys. Rev. B}, - Pages = {205111}, - Volume = {91}, - Year = {2015}} - -@article{HocHinBon-EPJST-14, - Author = {D. Hochstuhl and C. M. Hinz and M. Bonitz}, - Journal = {Eur. Phys. J Spec. Top.}, - Pages = {177}, - Volume = {223}, - Year = {2014}} - -@article{HohKoh-PR-64, - Author = {P. Hohenberg and W. Kohn}, - Journal = {Phys. Rev.}, - Pages = {B 864}, - Title = {Inhomogeneous Electron Gas}, - Volume = {{136}}, - Year = {1964}} - -@article{HolAraSin-PRB-79, - Author = {A. Holas and P. K. Aravind and K. S. Singwi}, - Journal = {Phys. Rev. B}, - Pages = {4912}, - Volume = {{20}}, - Year = {1979}} - -@article{HolBar-PRB-98, - Author = {B. Holm and U. von Barth}, - Journal = {Phys. Rev. B}, - Pages = {2108}, - Volume = {{57}}, - Year = {1998}} - -@incollection{Hol-INC-87, - Address = {New York}, - Author = {A. Holas}, - Booktitle = {Strongly Coupled Plasma Physics}, - Editor = {F. J. Rogers and H. E. Dewitt}, - Pages = {463-482}, - Publisher = {Plenum}, - Year = {1987}} - -@incollection{Hol-INC-91, - Address = {New York}, - Author = {A. Holas}, - Booktitle = {Electronic Structure of Solids}, - Editor = {P. Ziesche}, - Pages = {6-11}, - Publisher = {Nova Science}, - Year = {1991}} - -@article{HolPeg-JCP-18, - Author = {J. W. Hollett and N. Pegoretti}, - Journal = {J. Chem. Phys.}, - Pages = {164111}, - Volume = {148}, - Year = {2018}} - -@article{Hol-SA-63, - Author = {J. M. Hollas}, - Journal = {Spectrochim. Acta}, - Pages = {1425}, - Volume = {19}, - Year = {1963}} - -@article{HuaFilUmr-JCP-98, - Author = {C.-J. Huang and C. Filippi and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {8838}, - Volume = {{108}}, - Year = {1998}} - -@article{HuaUmrNig-JCP-97, - Author = {Chien-Jung Huang and C. J. Umrigar and M. P. Nightingale}, - Journal = {J. Chem. Phys.}, - Pages = {3007}, - Volume = {{107}}, - Year = {1997}} - -@book{HubHer-BOOK-79, - Author = {K. P. Huber and G. Herzberg}, - Publisher = {van Nostrand Reinhold Company}, - Title = {Molecular Spectra and Molecular Structure - IV. Constants of Diatomic Molecules}, - Year = {1979}} - -@article{hubac:8779, - Author = {Ivan Hubac and Jiri Pittner and Petr Carsky}, - Journal = {The Journal of Chemical Physics}, - Keywords = {coupled cluster calculations; error correction}, - Number = {20}, - Pages = {8779-8784}, - Publisher = {AIP}, - Title = {Size-extensivity correction for the state-specific multireference Brillouin--Wigner coupled-cluster theory}, - Url = {http://link.aip.org/link/?JCP/112/8779/1}, - Volume = {112}, - Year = {2000}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/112/8779/1}} - -@article{Hub-PRSL-58, - Author = {J. Hubbard}, - Journal = {Proc. R. Soc. London, Ser. A}, - Pages = {336}, - Volume = {{243}}, - Year = {1958}} - -@article{HueGri-CP-08, - Author = {Robert Huenerbein and Stefan Grimme}, - Journal = {Chem. Phys.}, - Pages = {362}, - Volume = {343}, - Year = {2008}} - -@misc{HuiCas-ARX-10, - Author = {M. Huix-Rotllant and M. E. Casida}, - Note = {\url{http://arxiv.org/abs/1008.1478}}, - Title = {Formal Foundations of Dressed Time-Dependent Density-Functional Theory for Many-Electron Excitations}} - -@phdthesis{Hui-THESIS-11, - Author = {M. Huix-Rotllant}, - School = {Universit\'e de Grenoble}, - Title = {Improved correlation kernels for linear-response time-dependent density-functional theory}, - Type = {{PhD thesis}}, - Year = {2011}} - -@article{IchUts-PRB-81, - Author = {S. Ichimaru and K. Utsumi}, - Journal = {Phys. Rev. B}, - Pages = {7385}, - Volume = {{24}}, - Year = {1981}} - -@article{IikTsuYanHir-JCP-01, - Author = {H. Iikura and T. Tsuneda and T. Yanai and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {3540}, - Volume = {{115}}, - Year = {2001}} - -@article{IkaNak-JCP-12, - Author = {Yasuhiro Ikabata1 and Hiromi Nakai}, - Journal = {J. Chem. Phys.}, - Pages = {124106}, - Volume = {137}, - Year = {2012}} - -@article{Inu-BCSJ-60, - Author = {K. Inuzuka}, - Journal = {Bull. Chem. Soc. Jpn.}, - Pages = {678}, - Volume = {33}, - Year = {1960}} - -@article{IreHenScu-JCP-11, - Author = {R. M. Irelan and T. M. Henderson and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {094105}, - Volume = {135}, - Year = {2011}} - -@article{Ish-CPL-89, - Author = {I. Ishida}, - Journal = {Chem. Phys. Lett.}, - Pages = {217}, - Volume = {158}, - Year = {1989}} - -@article{Har-IJQC-85, - Author = {K. Ishida}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {349}, - Volume = {28}, - Year = {1985}} - -@article{Har-IJQC-86, - Author = {K. Ishida}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {543}, - Volume = {30}, - Year = {1986}} - -@article{Ism-PRB-10, - Author = {S. Ismail-Beigi}, - Journal = {Phys. Rev. B}, - Pages = {195126}, - Volume = {81}, - Year = {2010}} - -@article{ivanov:10262, - Author = {Stanislav Ivanov and Kieron Burke and Mel Levy}, - Journal = {The Journal of Chemical Physics}, - Keywords = {density functional theory; perturbation theory; wave functions}, - Number = {21}, - Pages = {10262-10268}, - Publisher = {AIP}, - Title = {Exact high-density limit of correlation potential for two-electron density}, - Url = {http://link.aip.org/link/?JCP/110/10262/1}, - Volume = {110}, - Year = {1999}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/110/10262/1}} - -@article{IvaHirBar-JCP-02, - Author = {S. Ivanov and S. Hirata and R. J. Bartlett}, - Journal = {J. Chem. Phys.}, - Pages = {1269}, - Volume = {116}, - Year = {2002}} - -@article{IvaHirBar-PRL-99, - Author = {S. Ivanov and S. Hirata and R. J. Bartlett}, - Journal = {Phys. Rev. Lett.}, - Pages = {5455}, - Volume = {83}, - Year = {1999}} - -@article{IvaHirGraBar-JCP-03, - Author = {S. Ivanov and S. Hirata and I. Grabowski and R. J. Bartlett}, - Journal = {J. Chem. Phys.}, - Pages = {461}, - Volume = {118}, - Year = {2003}} - -@article{IvaLev-JCP-02, - Author = {Stanislav Ivanov and Mel Levy}, - Journal = {J. Chem. Phys.}, - Pages = {6924}, - Title = {Accurate correlation potentials from integral formulation of density functional perturbation theory}, - Volume = {116}, - Year = {2002}} - -@article{ivanov:7087, - Author = {Stanislav Ivanov and Mel Levy}, - Journal = {The Journal of Chemical Physics}, - Keywords = {ground states; HF calculations; perturbation theory}, - Number = {14}, - Pages = {7087-7093}, - Publisher = {AIP}, - Title = {Connections between ground-state energies from optimized-effective potential exchange-only and Hartree--Fock methods}, - Url = {http://link.aip.org/link/?JCP/119/7087/1}, - Volume = {119}, - Year = {2003}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/119/7087/1}} - -@article{IvaLev-JPCA-98, - Author = {Stanislav Ivanov and Mel Levy}, - Journal = {J. Phys. Chem. A}, - Pages = {3151}, - Volume = {102}, - Year = {1998}} - -@article{ivanov:6280, - Author = {Stanislav Ivanov and Roberto Lopez-Boada and Andreas Gorling and Mel Levy}, - Journal = {The Journal of Chemical Physics}, - Keywords = {Fourier transforms; wave functions; density functional theory}, - Number = {15}, - Pages = {6280-6286}, - Publisher = {AIP}, - Title = {Closed-form expression relating the second-order component of the density functional theory correlation energy to its functional derivative}, - Url = {http://link.aip.org/link/?JCP/109/6280/1}, - Volume = {109}, - Year = {1998}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/109/6280/1}} - -@phdthesis{Iva-THESIS-97, - Author = {S. Ivanov}, - School = {Tulane University}, - Title = {Correlation energies and pointwise identity for the DFT correlation potential in high-density scaling limit}, - Year = {1997}} - -@article{IzmStaScuDav-JCP-07, - Author = {A. F. Izmaylov and V. N. Staroverov and G. E. Scuseria and E. R. Davidson}, - Journal = {J. Chem. Phys.}, - Pages = {084113}, - Volume = {127}, - Year = {2007}} - -@article{JacDucBla-JCTC-15, - Author = {D. Jacquemin and I. Duchemin and X. Blase}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3290}, - Volume = {11}, - Year = {2015}} - -@article{JacPerCioAda-JCC-08, - Author = {D. Jacquemin and E. A. Perp\`ete and I. Ciofini and C. Adamo}, - Journal = {J. Comput. Chem.}, - Pages = {921}, - Volume = {29}, - Year = {2008}} - -@article{JacPerScaFriKobAda-JCP-07, - Author = {D. Jacquemin and E. A. Perp\`ete and G. Scalmani and M. J. Frisch and R. Kobayashi and C. Adamo}, - Journal = {J. Chem. Phys.}, - Pages = {144105}, - Volume = {126}, - Year = {2007}} - -@article{JacWatPerAda-JCTC-09, - Author = {D. Jacquemin and V. Wathelet and E. A. Perp\'ete and C. Adamo}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2420}, - Volume = {5}, - Year = {2009}} - -@article{JamCasSal-JCP-96, - Author = {C. Jamorski and M. E. Casida and D. R. Salahub}, - Journal = {J. Chem. Phys.}, - Pages = {5134}, - Volume = {104}, - Year = {1996}} - -@article{JanHenScu-JCP-09b, - Author = {B. G. Janesko and T. M. Henderson and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {034110}, - Volume = {131}, - Year = {2009}} - -@article{JanHenScu-JCP-09, - Author = {B. G. Janesko and T. M. Henderson and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {081105}, - Title = {Long-range-corrected hybrids including random phase approximation correlation}, - Volume = {130}, - Year = {2009}} - -@article{JanLiuAng-JCP-10, - Author = {G. Jansen and R.-F. Liu and J. G. \'Angyan}, - Journal = {J. Chem. Phys.}, - Pages = {154106}, - Volume = {133}, - Year = {2010}} - -@article{Jan-NC-62, - Author = {B. Jancovici}, - Journal = {Nuovo Cimento}, - Pages = {428}, - Volume = {XXV}, - Year = {1962}} - -@article{Jan-PRB-78, - Author = {J. F. Janak}, - Journal = {Phys. Rev. B}, - Pages = {7165}, - Volume = {18}, - Year = {1978}} - -@article{JanScu-JCP-09, - Author = {B. G. Janesko and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {154106}, - Volume = {131}, - Year = {2009}} - -@article{JanScu-PCCP-09, - Author = {B. G. Janesko and G. E. Scuseria}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {9677}, - Volume = {11}, - Year = {2009}} - -@article{JarDav-PRA-98, - Author = {A. A. Jarzecki and E. R. Davidson}, - Journal = {Phys. Rev. A}, - Pages = {1902}, - Title = {Ground-state energies of isoelectronic atomic series from density-functional theory: Exploring the accuracy of density functionals}, - Volume = {{58}}, - Year = {1998}} - -@article{JenAgr-CP-86, - Author = {H. J. Aa. Jensen and H. Agren}, - Journal = {Chem. Phys.}, - Pages = {229}, - Volume = {104}, - Year = {1986}} - -@article{JenAgr-CPL-84, - Author = {H. J. Aa. Jensen and H. Agren}, - Journal = {Chem. Phys. Lett.}, - Pages = {140}, - Volume = {110}, - Year = {1984}} - -@article{JenBun-JCP-88, - Author = {P. Jensen and P. R. Bunker}, - Journal = {J. Chem. Phys.}, - Pages = {1327}, - Volume = {89}, - Year = {1988}} - -@article{JenDyaSauFae-JCP-96, - Author = {H. J. Aa. Jensen and K. G. Dyall and T. Saue and K. F{\ae}gri}, - Journal = {J. Chem. Phys.}, - Pages = {4083}, - Volume = {104}, - Year = {1996}} - -@incollection{Jen-INC-94, - Address = {New York}, - Author = {H. J. Aa. Jensen}, - Booktitle = {Relativistic and Electron Correlation Effects in Molecules and Solids}, - Editor = {G. L. Malli}, - Pages = {179}, - Publisher = {Plenum}, - Year = {1994}} - -@article{JenJorAgr-JCP-87, - Author = {H. J. Aa. Jensen and P. Jorgensen and H. Agren}, - Journal = {J. Chem. Phys.}, - Pages = {451}, - Volume = {{87}}, - Year = {1987}} - -@article{JenJorAgrOls-JCP-88, - Author = {H. J. Aa. Jensen and P. J{\o}rgensen and H. Agren and J. Olsen}, - Journal = {J. Chem. Phys.}, - Pages = {3834}, - Volume = {{88}}, - Year = {1988}} - -@article{JenJor-JCP-84, - Author = {H. J. Aa. Jensen and P. J{\o}rgensen}, - Journal = {J. Chem. Phys.}, - Pages = {1204}, - Volume = {{80}}, - Year = {1984}} - -@article{JiaEng-JCP-07, - Author = {Hong Jiang and Eberhard Engel}, - Doi = {10.1063/1.2795707}, - Journal = {J. Chem. Phys.}, - Keywords = {density functional theory; eigenvalues and eigenfunctions; ground states; ionisation potential; orbital calculations; perturbation theory; potential energy functions}, - Pages = {184108}, - Title = {Random-phase-approximation-based correlation energy functionals: Benchmark results for atoms}, - Volume = {127}, - Year = {2007}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.2795707}} - -@article{JieNorSer-JCP-05, - Author = {A. Jiemchooroj and P. Norman and Bo E. Sernelius}, - Journal = {J. Chem. Phys.}, - Pages = {124312}, - Volume = {123}, - Year = {2005}} - -@article{JieNorSer-JCP-06, - Author = {A. Jiemchooroj and P. Norman and Bo E. Sernelius}, - Journal = {J. Chem. Phys.}, - Pages = {124306}, - Volume = {125}, - Year = {2006}} - -@article{JohBec-JCP-05b, - Author = {E. R. Johnson and A. D. Becke}, - Journal = {J. Chem. Phys.}, - Pages = {024101}, - Volume = {123}, - Year = {2005}} - -@article{JohMorCohYan-JCP-08, - Author = {E. R. Johnson and P. Mori-S{\'a}nchez and A. J. Cohen and W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {204112}, - Volume = {129}, - Year = {2008}} - -@article{JonGun-RMP-89, - Author = {R. O. Jones and O. Gunnarsson}, - Journal = {Rev. Mod. Phys.}, - Pages = {689}, - Volume = {{61}}, - Year = {1989}} - -@article{jones:325, - Author = {R. O. Jones}, - Journal = {The Journal of Chemical Physics}, - Keywords = {OZONE; SULFUR DIOXIDE; GROUND STATES; EXCITED STATES; ELECTRONIC STRUCTURE; CONFIGURATION INTERACTION; DISSOCIATION ENERGY; ATMOSPHERIC CHEMISTRY}, - Number = {1}, - Pages = {325-332}, - Publisher = {AIP}, - Title = {Energy surfaces of low-lying states of O[sub 3] and SO[sub 2]}, - Url = {http://link.aip.org/link/?JCP/82/325/1}, - Volume = {82}, - Year = {1985}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/82/325/1}} - -@article{JorSim-JCP-83, - Author = {P. J{\o}rgensen and J. Simons}, - Journal = {J. Chem. Phys.}, - Pages = {334}, - Volume = {79}, - Year = {1983}} - -@article{JouSri-JCP-98, - Author = {Daniel P. Joubert and G. P. Strivastava}, - Journal = {J. Chem. Phys.}, - Pages = {5212}, - Volume = {109}, - Year = {1998}} - -@article{JurSpoCerHob-PCCP-06, - Author = {P. Jure{\v c}ka and J. {\v S}poner and J. {\v C}ern{\'y} and P. Hobza}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {1985}, - Volume = {8}, - Year = {2006}} - -@article{KadVoo-JCP-10, - Author = {{B. Kaduk and T. Van Voorhis}}, - Journal = {J. Chem. Phys.}, - Pages = {061102}, - Volume = {133}, - Year = {2010}} - -@article{KalMusTou-JCP-19, - Author = {C. Kalai and B. Mussard and J. Toulouse}, - Doi = {10.1063/1.5108536}, - Journal = {J. Chem. Phys.}, - Pages = {074102}, - Title = {Range-separated double-hybrid density-functional theory with coupled-cluster and random-phase approximations}, - Volume = {151}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5108536}} - -@misc{KalMusTou-JJJ-19, - Author = {C. Kalai and B. Mussard and J. Toulouse}, - Note = {Range-separated double-hybrid density-functional theory with coupled-cluster and random-phase approximations \href{https://arxiv.org/abs/1905.01014}{arXiv:1905.01014}}} - -@article{KalTou-JCP-18, - Author = {C. Kalai and J. Toulouse}, - Doi = {10.1063/1.5025561}, - Journal = {J. Chem. Phys.}, - Pages = {164105}, - Title = {A general range-separated double-hybrid density-functional theory}, - Volume = {148}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5025561}} - -@misc{KalTou-JJJ-XX-note1, - Note = {The geometries are available in the Minnesota Database at http://comp.chem.umn.edu/db/.}} - -@misc{KalTou-JJJ-XX-note2, - Note = {The term ``range-separated double hybrid (RSDH)'' has already been used in Ref.~\onlinecite{SanCivUsvTouShaMas-JCP-15} to designate the RSH+MP2 method and in Refs.~\onlinecite{CorStoJenFro-PRA-13,CorFro-IJQC-14} to generically designate several kinds of range-separated MP2/DFT hybrids. In the present work, we use RSDH to designate the specific scheme corresponding to Eq.~(\ref{EmulRSDH}).}} - -@misc{KalTou-JJJ-XX-note3, - Note = {We use the AE49 set of Fast {\it et al.}~\cite{FasCorSanTru-JPCA-99} to facilitate comparisons with previous related works~\cite{ShaTouSav-JCP-11,SouShaTou-JCP-14,MusReiAngTou-JCP-15} where this set was used. We do not expect any special difficulties with the six molecules that have been dropped from the G2-1 set.}} - -@article{KamSekTsuHir-JCP-05, - Author = {M. Kamiya and H. Sekino and T. Tsuneda and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {234111}, - Volume = {122}, - Year = {2005}} - -@article{KamTsuHir-JCP-02, - Author = {M. Kamiya and T. Tsuneda and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {6010}, - Volume = {{117}}, - Year = {2002}} - -@article{KanBec-JCTC-10, - Author = {F. O. Kannemann and Axel D. Becke}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1081}, - Title = {{van der Waals interactions in density-functional theory: Intermolecular complexes}}, - Volume = {6}, - Year = {2010}} - -@article{KarDaoMar-CPL-11, - Author = {A. Karton and S. Daon and J. M. L. Martin}, - Journal = {Chem. Phys. Lett.}, - Pages = {165}, - Volume = {510}, - Year = {2011}} - -@article{Kar-JCP-03, - Author = {V. V. Karasiev}, - Journal = {J. Chem. Phys.}, - Pages = {8576}, - Volume = {118}, - Year = {2003}} - -@article{KarKroKum-JCP-13, - Author = {A. Karolewski and L. Kronik and S. K\"ummel}, - Journal = {J. Chem. Phys.}, - Pages = {204115}, - Volume = {138}, - Year = {2013}} - -@article{KarMar-JCP-11, - Author = {Amit Karton and J. M. L. Martin}, - Journal = {J. Chem. Phys.}, - Pages = {144119}, - Volume = {135}, - Year = {2011}} - -@article{KarTarLamSchMar-JPCA-08, - Author = {Amir Karton and Alex Tarnopolsky and Jean-Francois Lam\`ere and George C. Schatz and Jan M. L. Martin}, - Journal = {J. Phys. Chem. A}, - Pages = {12868}, - Volume = {112}, - Year = {2008}} - -@article{Kat-CPAM-57, - Author = {T. Kato}, - Journal = {Comm. Pure Appl. Math.}, - Pages = {151}, - Title = {{On the eigenfunctions of many-particle systems in quantum mechanics}}, - Volume = {10}, - Year = {1957}} - -@article{Kat-PRA-72, - Author = {J. Katriel}, - Journal = {Phys. Rev. A}, - Pages = {1990}, - Volume = {5}, - Year = {1972}} - -@article{Kat-PRA-80, - Author = {J. Katriel}, - Journal = {Phys. Rev. A}, - Pages = {1067}, - Volume = {21}, - Year = {1980}} - -@article{KauBauJun-JPB-89, - Author = {K. Kaufmann and W. Baumeistert and M. Jungen}, - Journal = {J. Phys. B}, - Pages = {2223}, - Title = {{Universal Gaussian basis sets for an optimum representation of Rydberg and continuum wavefunctions}}, - Volume = {22}, - Year = {1989}} - -@article{KauNorSai-JCP-13, - Author = {J. Kauczor and P. Norman and W. A. Saidi}, - Journal = {J. Chem. Phys.}, - Pages = {114107}, - Volume = {138}, - Year = {2013}} - -@article{KenDunHar-JCP-92, - Author = {R. A. Kendall and T. H. Dunning and R. J. Harrison}, - Journal = {J. Chem. Phys.}, - Pages = {6796}, - Volume = {96}, - Year = {1992}} - -@article{KhaHof-JCP-04, - Author = {Yuriy G. Khait and Mark R. Hoffmann}, - Journal = {J. Chem. Phys.}, - Pages = {5005}, - Title = {Multireference spin-adapted variant of density functional theory}, - Volume = {120}, - Year = {2004}} - -@article{KhaPanAve-IJQC-95, - Author = {Yu. G. Khait and A. I. Panin and A. S. Averyanov}, - Journal = {Int. J. Quantum Chem.}, - Pages = {329}, - Volume = {54}, - Year = {1995}} - -@article{Kim-PRA-73, - Author = {J. C. Kimball}, - Journal = {Phys. Rev. A}, - Pages = {1648}, - Volume = {{7}}, - Year = {1973}} - -@article{Kim-PRB-76, - Author = {J. C. Kimball}, - Journal = {Phys. Rev. B}, - Pages = {2371}, - Volume = {14}, - Year = {1976}} - -@article{KirBonRamChaMatSek-JCP-08, - Author = {Bernard Kirtman and Sean Bonness and Alejandro Ramirez-Solis and Benoit Champagne and Hironori Matsumoto and Hideo Sekino}, - Journal = {J. Chem. Phys.}, - Pages = {114108}, - Volume = {128}, - Year = {2008}} - -@incollection{KlaGil-AQC-12, - Author = {Shachar Klaiman and Ido Gilary}, - Booktitle = {Advances in Quantum Chemistry Vol. 63}, - Editor = {Cleanthes A. Nicolaides and Erkki Br\"andas and John R. Sabin}, - Pages = {1}, - Publisher = {Academic Press}, - Title = {On Resonance: A First Glance into the Behavior of Unstable States}, - Year = {2012}} - -@article{Kla-PRB-03, - Author = {T. Klamroth}, - Journal = {Phys. Rev. B}, - Pages = {245421}, - Volume = {68}, - Year = {2003}} - -@article{KlePic-JCP-76, - Author = {D. J. Klein and H. M. Pickett}, - Journal = {J. Chem. Phys.}, - Pages = {4811}, - Title = {{Nodal hypersurfaces and Anderson's random-walk simulation of the Schr\"odinger equation}}, - Volume = {64}, - Year = {1976}} - -@article{KliMic-JCP-12, - Author = {J. Klime{\v s} and A. Michaelides}, - Journal = {J. Chem. Phys.}, - Pages = {120901}, - Title = {Perspective: Advances and challenges in treating van der Waals dispersion forces in density functional theory}, - Volume = {137}, - Year = {2012}} - -@article{KloBakJorOlsHel-JPB-99, - Author = {W. Klopper and K. L. Bak and P. J{\o}rgensen and J. Olsen and T. Helgaker}, - Journal = {J. Phys. B}, - Pages = {R103}, - Volume = {32}, - Year = {1999}} - -@article{Klo-MP-01, - Author = {W. Klopper}, - Journal = {Mol. Phys.}, - Pages = {481}, - Volume = {99}, - Year = {2001}} - -@article{KloSam-JCP-02, - Author = {W. Klopper and C. M. Samson}, - Journal = {J. Chem. Phys.}, - Pages = {6397}, - Volume = {116}, - Year = {2002}} - -@article{KloTeaCorPedHel-CPL-11, - Author = {W. Klopper and A. M. Teale and S. Coriani and T. B. Pedersen and T. Helgaker}, - Journal = {Chem. Phys. Lett.}, - Pages = {147}, - Volume = {510}, - Year = {2011}} - -@incollection{KnoSchWer-INC-00, - Address = {J\"{u}lich}, - Author = {P. J. Knowles and M. Sch\"{u}tz and H.-J. Werner}, - Booktitle = {Modern Methods and Algorithms of Quantum Chemistry}, - Editor = {J. Grotendorst}, - Pages = {61-151}, - Publisher = {NIC}, - Title = {Ab Initio Methods for Electron Correlation in Molecules}, - Volume = {1}, - Year = {2000}} - -@article{KnoWer-CPL-88, - Author = {P. J. Knowles and H-J. Werner}, - Journal = {Chem. Phys. Lett.}, - Pages = {145}, - Volume = {{514}}, - Year = {1988}} - -@book{KocHol-BOOK-01, - Address = {New York}, - Author = {W. Koch and M. C. Holthausen}, - Publisher = {Wiley-VCH}, - Title = {A Chemist's Guide To Density Functional Theory}, - Year = {2001}} - -@article{Kog-JCP-01b, - Author = {T. Koga}, - Journal = {J. Chem. Phys.}, - Pages = {102}, - Volume = {114}, - Year = {2001}} - -@article{Kog-JCP-02, - Author = {T. Koga}, - Journal = {J. Chem. Phys.}, - Pages = {6614}, - Volume = {116}, - Year = {2002}} - -@article{Kog-JCP-90, - Author = {T. Koga}, - Journal = {J. Chem. Phys.}, - Pages = {5856}, - Volume = {93}, - Year = {1990}} - -@article{KogMatDehTha-JCP-99, - Author = {T. Koga and H. Matsuyama and S. Dehesa and A. J. Thakkar}, - Journal = {J. Chem. Phys.}, - Pages = {5763}, - Volume = {110}, - Year = {1999}} - -@article{KogMat-JCP-01, - Author = {T. Koga and H. Matsuyama}, - Journal = {J. Chem. Phys.}, - Pages = {3984}, - Volume = {115}, - Year = {2001}} - -@article{KogMat-JCP-97, - Author = {T. Koga and H. Matsuyama}, - Journal = {J. Chem. Phys.}, - Pages = {10062}, - Volume = {107}, - Year = {1997}} - -@article{KogTatTha-PRA-93, - Author = {T. Koga and H. Tatewaki and A. J. Thakkar}, - Journal = {Phys. Rev. A}, - Pages = {4510}, - Volume = {{47}}, - Year = {1993}} - -@article{KohBecPar-JPC-96, - Author = {W. Kohn and A. D. Becke and R. G. Parr}, - Journal = {J. Phys. Chem.}, - Pages = {12974}, - Volume = {{31}}, - Year = {1996}} - -@article{Koh-CPL-93, - Author = {W. Kohn}, - Journal = {Chem. Phys. Lett.}, - Pages = {167}, - Volume = {208}, - Year = {1993}} - -@misc{KohHan-JJJ-XXa, - Author = {W. Kohn and W. Hanke}, - Note = {unpublished}} - -@misc{KohHan-JJJ-XX, - Author = {W. Kohn and W. Hanke}, - Note = {unpublished}} - -@article{Koh-JCP-72, - Author = {A. D. Kohl}, - Journal = {J. Chem. Phys.}, - Pages = {4236}, - Volume = {56}, - Year = {1972}} - -@article{KohMeiMak-PRL-98, - Author = {W. Kohn and Y. Meir and D. E. Makarov}, - Journal = {Phys. Rev. Lett.}, - Pages = {4153}, - Volume = {80}, - Year = {1998}} - -@article{Koh-RMP-99, - Author = {W. Kohn}, - Journal = {Rev. Mod. Phys.}, - Pages = {1253}, - Title = {{Nobel Lecture: Electronic structure of matter - wave functions and density functionals}}, - Volume = {{71}}, - Year = {1999}} - -@article{KohSha-PR-65, - Author = {W. Kohn and L. J. Sham}, - Journal = {Phys. Rev.}, - Pages = {A1133}, - Volume = {140}, - Year = {1965}} - -@article{KolMit-RPP-11, - Author = {J. Koloren\v{c} and L. Mitas}, - Journal = {Rep. Prog. Phys.}, - Pages = {026502}, - Title = {{Applications of quantum Monte Carlo methods in condensed systems}}, - Volume = {74}, - Year = {2011}} - -@misc{KolReiAss-JJJ-XX, - Author = {A. Kollias and P. Reinhardt and R. Assaraf}, - Note = {unpublished.}} - -@article{KolTho-NL-12, - Author = {Kolb, Brian and Thonhauser, T.}, - Doi = {10.1142/S1793984412300063}, - Journal = {Nano Life}, - Number = {02}, - Pages = {1230006}, - Title = {Molecular biology at the quantum level: can modern density functional theory forge the path?}, - Volume = {02}, - Year = {2012}, - Bdsk-Url-1 = {https://doi.org/10.1142/S1793984412300063}} - -@article{KonHat-PRA-84, - Author = {Akihiro Kono and Shuzo Hattori}, - Journal = {Phys. Rev. A}, - Pages = {2981}, - Volume = {29}, - Year = {1984}} - -@article{KopPet-JPCA-02, - Author = {Jacek Koput and Kirk A. Peterson}, - Journal = {J. Phys. Chem. A}, - Pages = {9595}, - Volume = {106}, - Year = {2002}} - -@article{KorBouDucBlaMarBot-JCTC-14, - Author = {S. K\"orbel and P. Boulanger and I. Duchemin and X. Blase and M. A. L. Maarques and S. Botti}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3934}, - Volume = {10}, - Year = {2014}} - -@article{KorLucGri-JPCA-08, - Author = {M. Korth and A. L\"uchow and S. Grimme}, - Journal = {J. Phys. Chem. A}, - Pages = {2104}, - Volume = {112}, - Year = {2008}} - -@article{KosKos-JCP-86, - Author = {R. Kosloff and D. Kosloff}, - Journal = {J. Comput. Phys.}, - Pages = {363}, - Volume = {63}, - Year = {1986}} - -@article{KowYosVoo-JCP-11, - Author = {{T. Kowalczyk, S. R. Yorst, and T. Van Voorhis}}, - Journal = {J. Chem. Phys.}, - Pages = {054128}, - Volume = {134}, - Year = {2011}} - -@article{KozGruMar-JPCC-10, - Author = {Sebastian Kozuch and David Gruzman and Jan M. L. Martin}, - Journal = {J. Phys. Chem. C}, - Pages = {20801}, - Volume = {114}, - Year = {2010}} - -@article{KozMar-JCC-13, - Author = {S. Kozuch and J. M. L. Martin}, - Journal = {J. Comput. Chem.}, - Pages = {2327}, - Volume = {34}, - Year = {2013}} - -@article{KozMar-PCCP-11, - Author = {S. Kozuch and J. M. L. Martin}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {20104}, - Volume = {13}, - Year = {2011}} - -@article{Kra-CP-92, - Author = {E. Kraka}, - Journal = {Chem. Phys.}, - Pages = {141}, - Volume = {161}, - Year = {1992}} - -@incollection{KraCreNor-INC-92, - Address = {Chichester}, - Author = {E. Kraka and D. Cremer and S. Nordholm}, - Booktitle = {Molecules in Natural Science and Biomedicine}, - Editor = {Z.B. Maksic and M. Eckert-Maksic}, - Pages = {351}, - Publisher = {Ellis Horwood}, - Year = {1992}} - -@article{KraKlaSaa-JCP-05, - Author = {Pascal Krause and Tillmann Klamroth and Peter Saalfrank}, - Journal = {J. Chem. Phys.}, - Pages = {074105}, - Volume = {123}, - Year = {2005}} - -@article{KriLiIaf-PRA-92a, - Author = {J. B. Krieger and Y. Li and G. J. Iafrate}, - Journal = {Phys. Rev. A}, - Pages = {101}, - Volume = {45}, - Year = {1992}} - -@article{KriLiIaf-PRA-92, - Author = {J. B. Krieger and Y. Li and G. J. Iafrate}, - Journal = {Phys. Rev. A}, - Pages = {5453}, - Volume = {46}, - Year = {1992}} - -@article{Kro-AP-84, - Author = {E. Krotscheck}, - Journal = {Ann. Phys.}, - Pages = {1}, - Volume = {{155}}, - Year = {1984}} - -@article{Kro-JLTP-77, - Author = {E. Krotscheck}, - Journal = {J. Low Temp. Phys.}, - Pages = {199}, - Volume = {{27}}, - Year = {1977}} - -@article{KroKohQia-PRB-85, - Author = {E. Krotscheck and W. Kohn and G.-X. Qian}, - Journal = {Phys. Rev. B}, - Pages = {5693}, - Volume = {{32}}, - Year = {1985}} - -@article{Kro-PRA-77, - Author = {E. Krotscheck}, - Journal = {Phys. Rev. A}, - Pages = {397}, - Volume = {{15}}, - Year = {1977}} - -@article{KroSteRefBae-JCTC-12, - Author = {L. Kronik and T. Stein and S. Refaely-Abramson and R. Baer}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1515}, - Title = {Excitation gaps of finite-sized systems from Optimally-Tuned Range-Separated Hybrid Functionals}, - Volume = {8}, - Year = {2012}} - -@article{KruVydIzmScu-JCP-06, - Author = {Aliaksandr V. Krukau and Oleg A. Vydrov and Artur F. Izmaylov and and Gustavo E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {224106}, - Volume = {{125}}, - Year = {2006}} - -@article{KrySheByrHea-JCP-98, - Author = {Anna I. Krylov and C. David Sherrill and Edward F. C. Byrd and Martin Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {10669}, - Title = {Size-consistent wave functions for nondynamical correlation energy: The valence active space optimized orbital coupled-cluster doubles model}, - Volume = {109}, - Year = {1998}} - -@article{KryZie-JCTC-13, - Author = {M. Krykunov and T. Ziegler}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2761}, - Volume = {9}, - Year = {2013}} - -@article{KudScu-CPL-98, - Author = {K. N. Kudin and G. E. Scuseria}, - Journal = {Chem. Phys. Lett.}, - Pages = {611}, - Volume = {289}, - Year = {1998}} - -@article{KudScu-PRB-00, - Author = {K. N. Kudin and G. E. Scuseria}, - Journal = {Phys. Rev. B}, - Pages = {16440}, - Volume = {61}, - Year = {2000}} - -@article{Kuh-ZP-25, - Author = {W. Kuhn}, - Journal = {Z. Phys.}, - Pages = {408}, - Volume = {33}, - Year = {1925}} - -@article{Kul-PRA-87b, - Author = {Kenneth C. Kulander}, - Journal = {Phys. Rev. A}, - Pages = {2726}, - Volume = {36}, - Year = {1987}} - -@article{KulSau-CP-12, - Author = {O. Kullie and T. Saue}, - Journal = {Chem. Phys.}, - Pages = {54}, - Volume = {395}, - Year = {2012}} - -@article{KumKro-RMP-08, - Author = {S. K\"ummel and L. Kronik}, - Journal = {Rev. Mod. Phys.}, - Pages = {3}, - Volume = {80}, - Year = {2008}} - -@article{KurLawHea-MP-09, - Author = {Y. Kurzweil and K. V. Lawler and M. Head-Gordon}, - Journal = {Mol. Phys.}, - Pages = {2103}, - Title = {Analysis of multi-configuration density functional theory methods: theory and model application to bond-breaking}, - Volume = {107}, - Year = {2009}} - -@article{KurPer-PRB-99, - Author = {S. Kurth and J. P. Perdew}, - Journal = {Phys. Rev. B.}, - Pages = {10461}, - Volume = {59}, - Year = {1999}} - -@article{KutKlo-JCP-91, - Author = {W. Kutzelnigg and W. Klopper}, - Journal = {J. Chem. Phys.}, - Pages = {1985}, - Volume = {94}, - Year = {1991}} - -@article{KutMor-JCP-92, - Author = {{W. Kutzelnigg and J. D. Morgan III}}, - Journal = {J. Chem. Phys.}, - Pages = {4484}, - Volume = {96}, - Year = {1992}} - -@article{Kva-JCP-12, - Author = {S. Kvaal}, - Journal = {J. Chem. Phys.}, - Pages = {194109}, - Volume = {136}, - Year = {2012}} - -@article{LabZapCocVenTouCaiTaiLup-JCTC-18, - Author = {Marie Labeye and Felipe Zapata and Emanuele Coccia and Val\'erie V\'eniard and Julien Toulouse and J\'er\'emie Caillat and Richard Ta\"{\i}eb and Eleonora Luppi}, - Doi = {10.1021/acs.jctc.8b00656}, - Journal = {J. Chem. Theory Comput.}, - Pages = {5846}, - Title = {Optimal Basis Set for Electron Dynamics in Strong Laser Fields: The case of Molecular Ion H$_2$^+}, - Volume = {14}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1021/acs.jctc.8b00656}} - -@article{Lam-PRB-71, - Author = {J. Lam}, - Journal = {Phys. Rev. B}, - Pages = {3243}, - Volume = {{3}}, - Year = {1971}} - -@article{LanBau-JCP-91, - Author = {S. R. Langhoff and C. W. Bauschlicher}, - Journal = {J. Chem. Phys.}, - Pages = {5882}, - Volume = {95}, - Year = {1991}} - -@article{LanEliIshKal-JCP-00, - Author = {A. Landau and E. Eliav and Y. Ishikawa and U. Kaldor}, - Journal = {J. Chem. Phys.}, - Pages = {9905}, - Volume = {113}, - Year = {2000}} - -@article{LanMeh-PRB-83, - Author = {D. C. Langreth and M. J. Mehl}, - Journal = {Phys. Rev. B}, - Pages = {1809}, - Volume = {{28}}, - Year = {1983}} - -@article{LanMeh-PRL-81, - Author = {D. C. Langreth and M. J. Mehl}, - Journal = {Phys. Rev. Lett.}, - Pages = {446}, - Volume = {{47}}, - Year = {1981}} - -@article{LanPer-PRB-77, - Author = {D. C. Langreth and J. P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {2884}, - Volume = {{15}}, - Year = {1977}} - -@article{LanPer-PRB-80, - Author = {D. C. Langreth and J. P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {5469}, - Volume = {{21}}, - Year = {1980}} - -@article{LanPer-SSC-75, - Author = {D. C. Langreth and J. P. Perdew}, - Journal = {Solid State Commun.}, - Pages = {1425}, - Volume = {17}, - Year = {1975}} - -@article{LanRohHer-JPCB-08, - Author = {A. W. Lange and M. A. Rohrdanz and J. M. Hubert}, - Journal = {J. Phys. Chem. B}, - Pages = {6304}, - Volume = {112}, - Year = {2008}} - -@article{LanRotVrb-JCP-97, - Author = {Peter Langfelder and Stuart M. Rothstein and Jan Vrbikb}, - Journal = {J. Chem. Phys.}, - Pages = {8525}, - Volume = {107}, - Year = {1997}} - -@article{LawBauTouFilUmr-CPL-08, - Author = {{J. W. Lawson, C. W. Bauschlicher Jr, J. Toulouse, C. Filippi, C. J. Umrigar}}, - Journal = {Chem. Phys. Lett.}, - Pages = {170}, - Title = {{Quantum Monte Carlo study of the cooperative binding of NO2 to fragment models of carbon nanotubes}}, - Volume = {466}, - Year = {2008}} - -@article{LebHarGouAngKreDob-PRL-10, - Author = {S. Leb\`egue and J. Harl and T. Gould and J. G. \'Angy\'an and G. Kresse and J. F. Dobson}, - Journal = {Phys. Rev. Lett.}, - Pages = {196401}, - Volume = {105}, - Year = {2010}} - -@article{Lee-AQC-03, - Author = {Robert van Leeuwen}, - Journal = {Adv. Quantum Chem.}, - Pages = {24-94}, - Title = {Density functional approach to the many-body problem: key concepts and exact functionals}, - Volume = {43}, - Year = {2003}} - -@article{LeeBae-PRA-94, - Author = {{R. van Leeuwen and E. J. Baerends}}, - Journal = {Phys. Rev. A}, - Pages = {2421}, - Volume = {49}, - Year = {1994}} - -@article{LeeConNemLopDru-PRE-11, - Author = {{R. M. Lee, G. J. Conduit, N. Nemec, P. L\'opez Rios, and N. D. Drummond}}, - Journal = {Phys. Rev. E}, - Pages = {066706}, - Title = {{Strategies for improving the efficiency of quantum Monte Carlo calculations}}, - Volume = {83}, - Year = {2011}} - -@incollection{LeeDah-INC-94, - Address = {Amsterdam}, - Author = {{R. van Leeuwen and N. E. Dahlen}}, - Booktitle = {The Electron Liquid Paradigm in Condensed Matter Physics}, - Editor = {G. F. Giuliani and G. Vignale}, - Publisher = {IOS Press}, - Series = {Proceedings of the International School of Physics ``Enrico Fermi'', Vol. 157}, - Year = {2004}} - -@article{LeeGil-CPL-99, - Author = {A. M. Lee and P. M. W Gill}, - Journal = {Chem. Phys. Lett.}, - Pages = {271}, - Volume = {313}, - Year = {1999}} - -@article{LeeGriBae-ZPD-95, - Author = {{R. van Leeuwen, O. Gritsenko, and E. J. Baerends}}, - Journal = {Z. Phys. D}, - Pages = {229}, - Volume = {33}, - Year = {1995}} - -@article{LeeMelRap-JCP-05, - Author = {Myung Won Lee and Massimo Mella and Andrew M. Rappe}, - Journal = {J. Chem. Phys.}, - Pages = {244103}, - Volume = {112}, - Year = {2005}} - -@article{LeeMurKonLunLan-PRB-10, - Author = {K. Lee and E. D. Murray and L. Kong and B. I. Lundqvist and D. C. Langreth}, - Journal = {Phys. Rev. B}, - Pages = {081101}, - Title = {Higher-accuracy van der Waals density functional}, - Volume = {82}, - Year = {2010}} - -@article{LeeRic-CPL-88, - Author = {T. J. Lee and J. E. Rice}, - Journal = {Chem. Phys. Lett.}, - Pages = {406}, - Volume = {150}, - Year = {1988}} - -@phdthesis{Lee-THESIS-94, - Address = {Amsterdam}, - Author = {{R. van Leeuwen}}, - School = {Vrije Universitei}, - Title = {Kohn-Sham potentials in density functional theory}, - Type = {{PhD thesis}}, - Year = {1994}} - -@article{LeeYanPar-PRB-88, - Author = {C. Lee and W. Yang and R. G. Parr}, - Journal = {Phys. Rev. B}, - Pages = {785}, - Volume = {37}, - Year = {1988}} - -@article{LefWya-JCP-83, - Author = {Claude Leforestier and Robert E. Wyatt}, - Journal = {J. Chem. Phys.}, - Pages = {2334}, - Volume = {78}, - Year = {1983}} - -@article{LeiDobGro-JCC-99, - Author = {M. Lein and J. F. Dobson and E. K. U. Dobson}, - Journal = {J. Comput. Chem.}, - Pages = {12}, - Volume = {20}, - Year = {1999}} - -@article{LeiGroPer-PRB-00, - Author = {Manfred Lein and E. K. U. Gross and John P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {13431}, - Volume = {{61}}, - Year = {2000}} - -@article{LeiStoWerSav-CPL-97, - Author = {T. Leininger and H. Stoll and H.-J. Werner and A. Savin}, - Journal = {Chem. Phys. Lett.}, - Pages = {151}, - Title = {Combining long-range configuration interaction with short-range density functionals}, - Volume = {{275}}, - Year = {1997}} - -@article{LeiTou-AC-14, - Author = {T. Leininger and J. Toulouse}, - Journal = {L'Actualit\'e Chimique}, - Pages = {13-21}, - Title = {{Relever le d\'efi de la r\'esolution de l'\'equation de Schr\"odinger}}, - Volume = {382-383}, - Year = {2014}} - -@article{LemRogChe-PRA-95, - Author = {A. Lembarki and F. Rogemond and H. Chermette}, - Journal = {Phys. Rev. A}, - Pages = {3704}, - Volume = {52}, - Year = {1995}} - -@article{LenBal-JCP-83, - Author = {J. H. van Lenthe and G. G. Balint-Kurti}, - Journal = {J. Chem. Phys.}, - Pages = {5699}, - Volume = {78}, - Year = {1983}} - -@article{Len-JCP-80, - Author = {{B. H. Lengsfield III}}, - Journal = {J. Chem. Phys.}, - Pages = {382}, - Volume = {73}, - Year = {1980}} - -@article{LenLiu-JCP-81, - Author = {{B. H. Lengsfield III and B. Liu}}, - Journal = {J. Chem. Phys.}, - Pages = {478}, - Volume = {75}, - Year = {1981}} - -@article{LenLiu-JCP-81_fr, - Author = {{B. H. Lengsfield III et B. Liu}}, - Journal = {J. Chem. Phys.}, - Pages = {478}, - Volume = {75}, - Year = {1981}} - -@article{LenVerPul-MP-91, - Author = {J. H. van Lenthe and J. Verbeek and P. Pulay}, - Journal = {Mol. Phys.}, - Pages = {1159}, - Volume = {73}, - Year = {1991}} - -@article{LepMalPel-PRA-89, - Author = {M. B. Lepetit and J. P. Malrieu and M. Pelissier}, - Journal = {Phys. Rev. A}, - Pages = {981}, - Volume = {39}, - Year = {1989}} - -@article{LesKra-JCP-66, - Author = {W. A. Lester and M. Krauss}, - Journal = {J. Chem. Phys.}, - Pages = {207}, - Volume = {44}, - Year = {1966}} - -@article{LevBer-IJQC-68, - Author = {B. Levy and G. Berthier}, - Journal = {Int. J. Quantum Chem.}, - Pages = {307}, - Volume = {2}, - Year = {1968}} - -@incollection{Lev-INC-95, - Address = {New York}, - Author = {M. Levy}, - Booktitle = {Density Functional Theory}, - Editor = {E.K.U. Gross and R.M. Dreizler}, - Publisher = {Plenum Press}, - Title = {Coordinate scaling requirements for approximating exchange and correlation}, - Year = {1995}} - -@article{LevMarHan-JCP-96, - Author = {M. Levy and N. H. March and N. C. Handy}, - Journal = {J. Chem. Phys.}, - Pages = {1989}, - Volume = {104}, - Year = {1996}} - -@article{LevNag-PRL-99, - Author = {M. Levy and A. Nagy}, - Journal = {Phys. Rev. Lett.}, - Pages = {4361}, - Volume = {83}, - Year = {1999}} - -@incollection{LevPer-INC-85, - Address = {New York}, - Author = {M. Levy and J. P. Perdew}, - Booktitle = {Density Functional Methods in Physics}, - Editor = {R. M. Dreizler and J. da Providencia}, - Publisher = {Plenum}, - Year = {1985}} - -@article{LevPer-PRA-85, - Author = {M. Levy and J. P. Perdew}, - Journal = {Phys. Rev. A}, - Pages = {2010}, - Volume = {32}, - Year = {1985}} - -@article{LevPer-PRB-93, - Author = {M. Levy and J. P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {11638}, - Volume = {48}, - Year = {1993}} - -@article{LevPerSah-PRA-84, - Author = {M. Levy and J. P. Perdew and V. Sahni}, - Journal = {Phys. Rev. A}, - Pages = {2745}, - Volume = {30}, - Year = {1984}} - -@article{Lev-PNAS-79, - Author = {M. Levy}, - Journal = {Proc. Natl. Acad. Sci. U.S.A.}, - Pages = {6062}, - Volume = {76}, - Year = {1979}} - -@article{Lev-PRA-82, - Author = {M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {1200}, - Volume = {26}, - Year = {1982}} - -@article{Lev-PRA-91, - Author = {M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {4637}, - Volume = {43}, - Year = {1991}} - -@article{LevSov-PRA-84, - Author = {Z. H. Levine and P. Soven}, - Journal = {Phys. Rev. A}, - Pages = {625}, - Volume = {29}, - Year = {1984}} - -@article{LevYanPar-JCP-85, - Author = {M. Levy and W. Yang and R. G. Parr}, - Journal = {J. Chem. Phys.}, - Pages = {2334}, - Volume = {83}, - Year = {1985}} - -@article{LieCle-JCP-74a, - Author = {George C. Lie and Enrico Clementi}, - Journal = {J. Chem. Phys.}, - Pages = {1275}, - Title = {Study of the electronic structure of molecules. XXI. Correlation energy corrections as a functional of the Hartree-Fock density and its application to the hydrides of the second row atoms}, - Volume = {60}, - Year = {1974}} - -@article{LieCle-JCP-74b, - Author = {George C. Lie and Enrico Clementi}, - Journal = {J. Chem. Phys.}, - Pages = {1288}, - Title = {Study of the electronic structure of molecules. XXII. Correlation energy corrections as a functional of the Hartree-Fock type density and its application to the homonuclear diatomic molecules of the second row atoms}, - Volume = {60}, - Year = {1974}} - -@article{Lie-IJQC-83, - Author = {E. H. Lieb}, - Journal = {Int. J. Quantum Chem.}, - Pages = {243}, - Volume = {{24}}, - Year = {1983}} - -@article{LieOxf-IJQC-81, - Author = {E. H. Lieb and S. Oxford}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {427}, - Volume = {{19}}, - Year = {1981}} - -@misc{lifetimes-note1, - Note = {For $\ell=0$, $R_2(r)$ only diverges as $1/r$ at $r=0$ which is normalizable, i.e. $\int_0^\infty \text{d}r r^2 |R_2(r)|^2 < \infty$. However, even in this case, the expectation value of the Hamiltonian operator is infinite. For $\ell \geq 1$, $R_2(r)$ is not even normalizable.}} - -@misc{lifetimes-note2, - Note = {The general solution of the Schr\"odinger equation given in Eqs.~(\ref{solR})-(\ref{solR2}) is valid for $Z\not=0$. For $Z=0$, $R_1(r)$ in Eq.~(\ref{solR1}) becomes identically zero, and should be replaced by a function which has the same expression as $R_2(r)$ with the substitution $\sqrt{-2E} \to -\sqrt{-2E}$. The continuum scattering states are then obtained as a linear combination of these two functions. However, our analysis of complex-energy states remains unchanged. Thus, our procedure for determining the lifetimes is still valid for $Z=0$.}} - -@misc{lifetimes-note3, - Note = {Because we do not impose spherical symmetry in our calculations, we do not have exactly degenerate s, p, and d states.}} - -@article{LikMorSen-PRB-97, - Author = {C. N. Likos and S. Moroni and G. Senatore}, - Journal = {Phys. Rev. B}, - Pages = {8867}, - Volume = {{55}}, - Year = {1997}} - -@article{LilTavRotSeb-PRL-04, - Author = {O. A. von Lilienfeld and I. Tavernelli and U. Rothlisberger}, - Journal = {Phys. Rev. Lett.}, - Pages = {153004}, - Volume = {93}, - Year = {2004}} - -@article{LimCarLuoMaOlsTruGag-JCTC-14, - Author = {{G. Li Manni, R. K. Carlson, S. Luo, D. Ma, J. Olsen, D. G. Truhlar, and L. Gagliardi}}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3669}, - Volume = {10}, - Year = {2014}} - -@article{LinRyuLiu-JCP-91, - Author = {R. Lindh and U. Ryu and B. Liu}, - Journal = {J. Chem. Phys.}, - Pages = {5889}, - Volume = {{95}}, - Year = {1991}} - -@article{LinSal-AQC-03, - Author = {Ingvar Lindgren and Sten Salomonson}, - Journal = {Adv. Quantum Chem.}, - Pages = {95-117}, - Title = {Differentiability in density-functional theory}, - Volume = {43}, - Year = {2003}} - -@article{LinTsaLiCha-JCP-12, - Author = {Y.-S. Lin and C.-W. Tsai and G.-D. Li and J.-D. Chai}, - Journal = {J. Chem. Phys.}, - Pages = {154109}, - Volume = {136}, - Year = {2012}} - -@article{LinZhaRap-JCP-00, - Author = {Xi Lin and Hongkai Zhang and Andrew M. Rappe}, - Journal = {J. Chem. Phys.}, - Pages = {2650}, - Volume = {112}, - Year = {2000}} - -@article{LiuEggRefKroNea-JCP-17, - Author = {Zhen-Fei Liu and David A. Egger and Sivan Refaely-Abramson and Leeor Kronik and Jeffrey B. Neaton}, - Journal = {J. Chem. Phys.}, - Pages = {092326}, - Volume = {146}, - Year = {2017}} - -@article{LiuParNag-PRA-95, - Author = {S. Liu and R. G. Parr and A. Nagy}, - Journal = {Phys. Rev. A}, - Pages = {2645}, - Volume = {52}, - Year = {1995}} - -@article{LivBae-PCCP-07, - Author = {E. Livshits and R. Baer}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {2932}, - Volume = {9}, - Year = {2007}} - -@article{LjuKovFerFoeSan-PRB-15, - Author = {M. P. Ljungberg and P. Koval and F. Ferrari and D. Foerster and D. S\'anchez-Portal}, - Journal = {Phys. Rev. B}, - Pages = {075422}, - Volume = {92}, - Year = {2015}} - -@article{LocHea-JCP-07, - Author = {Rohini C. Lochan and Martin Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {164101}, - Volume = {126}, - Year = {2007}} - -@article{Lon-DFS-65, - Author = {H. C. Longuet-Higgins}, - Journal = {Discuss. Faraday Soc.}, - Pages = {7}, - Volume = {40}, - Year = {1965}} - -@article{Lon-ZP-30, - Author = {F. London}, - Journal = {Z. Physik}, - Pages = {245}, - Volume = {63}, - Year = {1930}} - -@article{LooGil-WIRES-16, - Author = {Pierre-Francois Loos and Peter M. W. Gill}, - Journal = {WIREs Comput. Mol. Sci.}, - Note = {doi: 10.1002/wcms.1257}, - Pages = {410}, - Title = {The uniform electron gas}, - Volume = {6}, - Year = {2016}} - -@article{LooPraSceGinTou-ARX-19, - Author = {P.-F. Loos and B. Pradines and A. Scemama and E. Giner and J. Toulouse}, - Journal = {arXiv:1910.12238}, - Title = {A density-based basis-set incompleteness correction for GW methods}} - -@article{LooPraSceTouGin-JPCL-19, - Author = {P.-F. Loos and B. Pradines and A. Scemama and J. Toulouse and E. Giner}, - Doi = {10.1021/acs.jpclett.9b01176}, - Journal = {J. Phys. Chem. Lett.}, - Pages = {2931}, - Title = {A density-based basis-set correction for wave function theory}, - Volume = {10}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1021/acs.jpclett.9b01176}} - -@article{LopGov-JCTC-11, - Author = {K. Lopata and N. Govind}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1344}, - Title = {Modeling Fast Electron Dynamics with Real-Time Time-Dependent Density Functional Theory: Application to Small Molecules and Chromophores}, - Volume = {7}, - Year = {2011}} - -@article{LopGov-JCTC-13, - Author = {K. Lopata and N. Govind}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4939}, - Volume = {9}, - Year = {2013}} - -@article{LopMaDruTowNee-PRE-06, - Author = {{P. L\'opez Rios, A. Ma, N. D. Drummond, M. D. Towler, and R. J. Needs}}, - Journal = {Phys. Rev. E}, - Pages = {066701}, - Title = {{Inhomogeneous backflow transformations in quantum Monte Carlo calculations}}, - Volume = {74}, - Year = {2006}} - -@article{LopRamGarFer-JCP-87, - Author = {{R. L\'opez, G. Ram\'irez, J. M. Garc\'ia de la Vega and J. Fern\'andez Rico}}, - Journal = {J. chim. phys.}, - Pages = {695}, - Volume = {{84}}, - Year = {1987}} - -@article{LosFdeAguMar-JPC-07, - Author = {{A. M. Losa, I. Fdez.-Galv\'an, M. A. Aguilar, and M. E. Mart\'in}}, - Journal = {J. Phys. Chem. B}, - Pages = {9864}, - Volume = {111}, - Year = {2007}} - -@article{LotBar-JCP-11, - Author = {V. Lotrich and R. J. Bartlett}, - Journal = {J. Chem. Phys.}, - Pages = {184108}, - Volume = {134}, - Year = {2011}} - -@article{Low-AP-56, - Author = {P.-O. L\"owdin}, - Journal = {Adv. Phys.}, - Pages = {1}, - Volume = {5}, - Year = {1956}} - -@article{Low-JCP-50, - Author = {P.-O. L\"owdin}, - Journal = {J. Chem. Phys.}, - Pages = {365}, - Volume = {18}, - Year = {1950}} - -@article{Low-RMP-63, - Author = {P.-O. L\"owdin}, - Journal = {Rev. Mod. Phys.}, - Pages = {496}, - Volume = {35}, - Year = {1963}} - -@article{LowShu-PR-56, - Author = {P.-O. L\"owdin and H. Shull}, - Journal = {Phys. Rev.}, - Pages = {1730}, - Volume = {101}, - Year = {1956}} - -@article{LufRefPacResRamKroPus-PRB-14, - Author = {D. L\"uftner and Sivan Refaely-Abramson and Michael Pachler and Roland Resel and Michael G. Ramsey and Leeor Kronik and Peter Puschnig}, - Journal = {Phys. Rev. B}, - Pages = {075204}, - Volume = {90}, - Year = {2014}} - -@article{LuLiRocGal-PRL-09, - Author = {Deyu Lu and Yan Li and Dario Rocca and Giulia Galli}, - Journal = {Phys. Rev. Lett.}, - Pages = {206411}, - Volume = {102}, - Year = {2009}} - -@article{LuNguGal-JCP-10, - Author = {Deyu Lu and Huy-Viet Nguyen and Giulia Galli}, - Journal = {J. Chem. Phys.}, - Pages = {154110}, - Volume = {133}, - Year = {2010}} - -@article{LupHea-JCP-13, - Author = {E. Luppi and M. Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {164121}, - Title = {{The role of Rydberg and continuum levels in computing high harmonic generation spectra of the hydrogen atom using time-dependent configuration interaction}}, - Volume = {139}, - Year = {2013}} - -@article{Lut-ZPC-23, - Author = {A. Luthy}, - Journal = {Z. Phys. Chem., Stoechiom. Verwandtschaftsl.}, - Pages = {284}, - Volume = {107}, - Year = {1923}} - -@article{LynTru-JPCA-03, - Author = {B. J. Lynch and D. G. Truhlar}, - Journal = {J. Phys. Chem. A}, - Pages = {8996}, - Title = {Small Representative Benchmarks for Thermochemical Calculations}, - Volume = {107}, - Year = {2003}} - -@misc{LynZhaTru-JJJ-XX, - Note = {The geometries are available in the Minnesota Databases for Chemistry and Solid-State Physics at http://comp.chem.umn.edu/db/.}} - -@article{MaBru-PR-68, - Author = {S.-K. Ma and K. A. Brueckner}, - Journal = {Phys. Rev.}, - Pages = {165}, - Volume = {{165}}, - Year = {1968}} - -@article{MacVos-JPC-79, - Author = {A. H. MacDonald and S. H. Vosko}, - Journal = {J. Phys. C}, - Pages = {2977}, - Volume = {12}, - Year = {1979}} - -@article{MaDruTowNee-PRE-05, - Author = {A. Ma and N. D. Drummond and M. D. Towler and R. J. Needs}, - Journal = {Phys. Rev. E}, - Pages = {066704}, - Volume = {71}, - Year = {2005}} - -@book{Mah-BOOK-09, - Address = {Princeton}, - Author = {Gerald D. Mahan}, - Publisher = {Princeton University Press}, - Title = {Quantum Mechanics in a Nutshell}, - Year = {2009}} - -@article{MaiZhaCavBur-JCP-04, - Author = {N. T. Maitra and F. Zhang and R. J. Cave and K. Burke}, - Journal = {J. Chem. Phys.}, - Pages = {5932}, - Volume = {120}, - Year = {2004}} - -@article{MalMcd-CPL-98, - Author = {N. O. J. Malcolm and J. J. W. McDouall}, - Journal = {Chem. Phys. Lett.}, - Pages = {121}, - Volume = {282}, - Year = {1998}} - -@article{MalMcd-JPC-96, - Author = {N. O. J. Malcolm and J. J. W. McDouall}, - Journal = {J. Phys. Chem.}, - Pages = {10131}, - Volume = {100}, - Year = {1996}} - -@article{MalPenYanBalHol-TCA-14, - Author = {A. Malek and D. Peng and W. Yang and R. Balawender and A. Holas}, - Journal = {Theor. Chem. Acc.}, - Pages = {1559}, - Volume = {133}, - Year = {2014}} - -@article{ManLuc-JCP-01, - Author = {S. Manten and A. L\"uchow}, - Journal = {J. Chem. Phys.}, - Pages = {5362}, - Volume = {115}, - Year = {2001}} - -@article{MarAzaCasSor-JCP-09, - Author = {M. Marchi and S. Azadi and M. Casula and S. Sorella}, - Journal = {J. Chem. Phys.}, - Pages = {154116}, - Title = {Correlated geminal wave function for molecules: An efficient resonating valence bond approach}, - Volume = {131}, - Year = {2009}} - -@article{MarCasMalMulBot-JCP-07, - Author = {M. A. L. Marques and A. Castro and G. Malloci and G. Mulas and S. Botti}, - Journal = {J. Chem. Phys.}, - Pages = {014107}, - Volume = {127}, - Year = {2007}} - -@article{Mar-CPL-96, - Author = {J. M. L. Martin}, - Journal = {Chem. Phys. Lett.}, - Pages = {669}, - Volume = {259}, - Year = {1996}} - -@article{MarGarRub-PRL-06, - Abstract = {We present a first-principles description of anisotropic materials - characterized by having both weak (dispersionlike) and strong covalent - bonds, based on the adiabatic-connection fluctuation-dissipation - theorem with density functional theory. For hexagonal boron nitride - the in-plane and out-of-plane bonding as well as vibrational dynamics - are well described both at equilibrium and when the layers are pulled - apart. Bonding in covalent and ionic solids is also described. The - formalism allows us to ping down the deficiencies of common exchange-correlation - functionals and provides insight toward the inclusion of dispersion - interactions into the correlation functional.}, - Author = {Marini, A. and Garc\'ia-Gonz\'alez, P. and Rubio, A.}, - Journal = {Phys. Rev. Lett.}, - Pages = {136404}, - Title = {First-Principles Description of Correlation Effects in Layered Materials}, - Volume = {96}, - Year = {2006}} - -@article{MarHea-JCP-16, - Author = {Narbe Mardirossian and Martin Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {214110}, - Volume = {144}, - Year = {2016}} - -@article{MarHea-JCP-18, - Author = {Narbe Mardirossian and Martin Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {241736}, - Volume = {148}, - Year = {2018}} - -@article{MarHea-PCCP-14, - Author = {Narbe Mardirossian and Martin Head-Gordon}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {9904}, - Volume = {16}, - Year = {2014}} - -@article{MarHeiKle-WIRES-18, - Author = {Christel M. Marian and Adrian Heil and Martin Kleinschmidt}, - Journal = {WIREs Comput. Mol. Sci.}, - Note = {doi: 10.1002/wcms.1394}, - Pages = {e1394}, - Title = {The DFT/MRCI method}, - Year = {2018}} - -@article{MarLosFdeAgu-JCP-04, - Author = {{M. E. Mart\'in, A. M. Losa, I. Fdez.-Galv\'an, and M. A. Aguilar}}, - Journal = {J. Chem. Phys.}, - Pages = {3710}, - Volume = {121}, - Year = {2004}} - -@article{MarMea-JCP-78, - Author = {D. J. Margoliash and W. J. Meath}, - Journal = {J. Chem. Phys.}, - Pages = {1426}, - Volume = {68}, - Year = {1978}} - -@article{MaRohMol-JCTC-10, - Author = {Y. Ma and M. Rohlfing and C. Molteni}, - Journal = {J. Chem. Theory Comput.}, - Pages = {257}, - Volume = {6}, - Year = {2010}} - -@article{MaRohMol-PRB-09, - Author = {Y. Ma and M. Rohlfing and C. Molteni}, - Journal = {Phys. Rev. B}, - Pages = {241405}, - Volume = {80}, - Year = {2009}} - -@article{Mar-PR-58, - Author = {N. H. March}, - Journal = {Phys. Rev.}, - Pages = {604}, - Volume = {{110}}, - Year = {1958}} - -@book{MarReiCep-BOOK-16, - Author = {Richard M. Martin and Lucia Reining and David M. Ceperley}, - Publisher = {Cambridge University Press}, - Title = {Interacting Electrons: Theory and Computational Approaches}, - Year = {2016}} - -@article{MarWer-JPCA-09, - Author = {O. Marchetti and H.-J. Werner}, - Journal = {J. Phys. Chem. A}, - Pages = {11580}, - Volume = {113}, - Year = {2009}} - -@article{Math10-PROG-15, - Note = {{Wolfram Research, Inc., Mathematica, Version 10.3, Champaign, IL (2015)}}} - -@article{Math9-PROG-12, - Note = {{Wolfram Research, Inc., Mathematica, Version 9.0, Champaign, IL (2012)}}} - -@article{MatKogRomDeh-PRA-98, - Author = {H. Matsuyama and T. Koga and E. Romera and J. S. Dehesa}, - Journal = {Phys. Rev. A}, - Pages = {1759}, - Volume = {57}, - Year = {1998}} - -@article{MatKoh-JCP-01, - Author = {Ann E. Mattsson and Walter Kohn}, - Journal = {The Journal of Chemical Physics}, - Keywords = {surface energy; density functional theory; errors; surface potential; jellium}, - Number = {8}, - Pages = {3441-3443}, - Publisher = {AIP}, - Title = {An energy functional for surfaces}, - Url = {http://link.aip.org/link/?JCP/115/3441/1}, - Volume = {115}, - Year = {2001}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/115/3441/1}} - -@article{Mat-S-02, - Author = {A. E. Mattson}, - Journal = {Science}, - Pages = {759}, - Volume = {298}, - Year = {2002}} - -@article{MccStrWis-PRA-91, - Author = {C. W. McCurdy and C. K. Stroud and M. K. Wisinski}, - Journal = {Phys. Rev. A}, - Pages = {5980}, - Volume = {43}, - Year = {1991}} - -@article{Mcd-MP-03, - Author = {J. J. W. McDouall}, - Journal = {Mol. Phys.}, - Pages = {361}, - Title = {Combining two-body density functionals with multiconfigurational wavefunctions: diatomic molecules}, - Volume = {101}, - Year = {2003}} - -@article{MclBal-RMP-64, - Author = {McLachlan, A. D. and Ball, M. A.}, - Doi = {10.1103/RevModPhys.36.844}, - Journal = {Rev. Mod. Phys.}, - Pages = {844-855}, - Title = {Time-dependent Hartree-Fock Theory for Molecules}, - Volume = {36}, - Year = {1964}, - Bdsk-Url-1 = {https://doi.org/10.1103/RevModPhys.36.844}} - -@book{McW-BOOK-92, - Address = {London}, - Author = {R. McWeeny}, - Publisher = {Academic Press}, - Title = {Methods of Molecular Quantum Mechanics. Second Edition}, - Year = {1992}} - -@article{Mcw-CCA-84, - Author = {R. McWeeny}, - Journal = {Croat. Chem. Acta}, - Pages = {865}, - Volume = {57}, - Year = {1984}} - -@article{MehCasGor-PCCP-18, - Author = {N. Mehta and M. Casanova-P\'aez and Lars Goerigk}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {23175}, - Volume = {20}, - Year = {2018}} - -@article{MelSan-PRE-05, - Author = {Melko, R. G. and Sandvik, A. W.}, - Doi = {10.1103/PhysRevE.72.026702}, - Issue = {2}, - Journal = {Phys. Rev. E}, - Numpages = {22}, - Pages = {026702}, - Publisher = {American Physical Society}, - Title = {{Stochastic series expansion algorithm for the $S=1∕2$ $XY$ model with four-site ring exchange}}, - Url = {http://link.aps.org/doi/10.1103/PhysRevE.72.026702}, - Volume = {72}, - Year = {2005}, - Bdsk-Url-1 = {http://link.aps.org/doi/10.1103/PhysRevE.72.026702}, - Bdsk-Url-2 = {https://doi.org/10.1103/PhysRevE.72.026702}} - -@article{MenAnd-JCP-81, - Author = {F. Mentch and J. B. Anderson}, - Journal = {J. Chem. Phys.}, - Pages = {6307}, - Volume = {74}, - Year = {1981}} - -@incollection{MerValUga-INC-03, - Address = {Dordrecht}, - Author = {J. M. Mercero and E. Valderrama and J. M. Ugalde}, - Booktitle = {NATO-ASI Series in Metal-Ligand Interaction in Molecular-, Nano-, Micro, and Macro-systems in Complex Environments}, - Editor = {N. Russo, D. R. Salahub and M. Witko}, - Publisher = {Kluwer Academic Publishers}, - Year = {2003}} - -@article{MetRosRosTelTel-JCP-53, - Author = {N. Metropolis and A. W. Rosenbluth and M. N. Rosenbluth and A. H. Teller and E. Teller}, - Journal = {J. Chem. Phys.}, - Pages = {1087}, - Title = {{Equations of state calculations by fast computing machines}}, - Volume = {21}, - Year = {1953}} - -@article{MeyMulSch-JMS-96, - Author = {H. Meyer and T. M\"uller and A. Schweig}, - Journal = {J. Mol. Struct. (Theochem)}, - Pages = {55}, - Volume = {306}, - Year = {1996}} - -@article{MezCsoRuzKal-JCTC-15, - Author = {P. D. Mezei and G. I. Csonka and A. Ruzsinszky and M. K\'allay}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4615}, - Volume = {11}, - Year = {2015}} - -@article{MezCsoRuzKal-JCTC-17, - Author = {P. D. Mezei and G. I. Csonka and A. Ruzsinszky and M. K\'allay}, - Journal = {J. Chem. Theory Comput.}, - Pages = {796}, - Volume = {13}, - Year = {2017}} - -@article{MieSavStoPre-CPL-89, - Author = {B. Miehlich and A. Savin and H. Stoll and H. Preuss}, - Journal = {Chem. Phys. Lett.}, - Pages = {200}, - Volume = {157}, - Year = {1989}} - -@article{MieStoSav-MP-97, - Author = {B. Miehlich and H. Stoll and A. Savin}, - Journal = {Mol. Phys.}, - Pages = {527}, - Title = {A correlation-energy density functional for multideterminantal wavefunctions}, - Volume = {{91}}, - Year = {1997}} - -@article{Mil-PR-65, - Author = {{W. L. McMillan}}, - Journal = {Phys. Rev.}, - Pages = {A442}, - Title = {{Ground state of liquid He$^4$}}, - Volume = {138}, - Year = {1965}} - -@article{MisJezSza-PRL-03, - Author = {A. J. Misquitta and B. Jeziorski and K. Szalewicz}, - Journal = {Phys. Rev. Lett.}, - Pages = {033201}, - Volume = {91}, - Year = {2003}} - -@article{Mit-PRA-81, - Author = {M. H. Mittleman}, - Journal = {Phys. Rev. A}, - Pages = {1167}, - Volume = {24}, - Year = {1981}} - -@article{MiyAryKotSchUsuTer-PRB-02, - Author = {Miyake, T. and Aryasetiawan, F. and Kotani, T. and Schilfgaarde, M. v. and Usuda, M. and Terakura, K.}, - Journal = {Phys. Rev. B.}, - Pages = {245103}, - Title = {Total energy of solids: An exchange and random-phase approximation correlation study}, - Volume = {66}, - Year = {2002}} - -@book{Moi-BOOK-11, - Address = {Cambridge}, - Author = {Nimrod Moiseyev}, - Publisher = {Cambridge University Press}, - Title = {Non-Hermitian Quantum Mechanics}, - Year = {2011}} - -@article{MolPle-PR-34, - Author = {C. M{\o}ller and M. S. Plesset}, - Journal = {Phys. Rev.}, - Pages = {618}, - Volume = {46}, - Year = {1934}} - -@misc{Molpro-PROG-02, - Address = {Birmingham, UK}, - Author = {R. D. Amos and A. Bernhardsson and A. Berning and P. Celani and D. L. Cooper and M. J. O. Deegan and A. J. Dobbyn and F. Eckert and C. Hampel and G. Hetzer and P. J. Knowles and T. Korona and R. Lindh and A. W. Lloyd and S. J. {McNicholas} and F. R. Manby and W. Meyer and M. E. Mura and A. Nicklass and P. Palmieri and R. Pitzer and G. Rauhut and M. {Sch\"{u}tz} and U. Schumann and H. Stoll and A. J. Stone and R. Tarroni and T. Thorsteinsson and H.-J. Werner}, - Title = {MOLPRO, a package of ab initio programs designed by {H.-J.~Werner} and {P.~J. Knowles}, version 2002.2}, - Year = {2002}} - -@misc{Molpro-PROG-10, - Address = {Cardiff, UK}, - Author = {H.-J. Werner and P. J. Knowles and G. Knizia and F. R. Manby and M. {Sch\"{u}tz} and P. Celani and T. Korona and R. Lindh and A. Mitrushenkov and G. Rauhut and K. R. Shamasundar and T. B. Adler and R. D. Amos and A. Bernhardsson and A. Berning and D. L. Cooper and M. J. O. Deegan and A. J. Dobbyn and F. Eckert and E. Goll and C. Hampel and A. Hesselmann and G. Hetzer and T. Hrenar and G. Jansen and C. K\"oppl and Y. Liu and A. W. Lloyd and R. A. Mata and A. J. May and S. J. McNicholas and W. Meyer and M. E. Mura and A. Nicklass and D. P. O'Neill and P. Palmieri and K. Pfl\"uger and R. Pitzer and M. Reiher and T. Shiozaki and H. Stoll and A. J. Stone and R. Tarroni and T. Thorsteinsson and M. Wang and A. Wolf}, - Note = {see http://www.molpro.net}, - Title = {MOLPRO, version 2010.1, a package of ab initio programs}, - Year = 2010} - -@misc{Molproshort-PROG-02, - Address = {Birmingham, UK}, - Title = {MOLPRO, a package of ab initio programs designed by {H.-J.~Werner} and {P.~J. Knowles}, version 2002.2}, - Year = {2002}} - -@misc{Molproshort-PROG-08, - Address = {Cardiff, UK}, - Author = {H.-J. Werner and P. J. Knowles and R. Lindh and F. R. Manby and M. {Sch\"{u}tz} and others}, - Note = {see www.molpro.net}, - Title = {MOLPRO, version 2008.2, a package of ab initio programs}, - Year = {2008}} - -@misc{Molproshort-PROG-10, - Author = {{H.-J. Werner, P. J. Knowles, G. Knizia, F. R. Manby, M. {Sch\"{u}tz}, and others}}, - Note = {Cardiff, UK, 2010, see \url{http://www.molpro.net}}, - Title = {MOLPRO, version 2010.1, a package of ab initio programs}} - -@misc{Molproshort-PROG-12, - Author = {{H.-J. Werner, P. J. Knowles, G. Knizia, F. R. Manby, M. {Sch\"{u}tz}, and others}}, - Note = {Cardiff, UK, 2012, see \url{http://www.molpro.net}}, - Title = {MOLPRO, version 2012.1, a package of ab initio programs}} - -@misc{Molproshort-PROG-15, - Author = {{H.-J. Werner, P. J. Knowles, G. Knizia, F. R. Manby, M. {Sch\"{u}tz}, and others}}, - Note = {{Cardiff, UK, 2015, see \url{http://www.molpro.net}}}, - Title = {{MOLPRO, version 2015.1, a package of ab initio programs}}} - -@misc{Molproshort-PROG-19, - Author = {{H.-J. Werner, P. J. Knowles, G. Knizia, F. R. Manby, M. {Sch\"{u}tz}, and others}}, - Note = {{Cardiff, UK, 2019, see \url{http://www.molpro.net}}}, - Title = {{MOLPRO, version 2019.1, a package of ab initio programs}}} - -@misc{Molproweb-PROG-XX, - Note = {\url{http://www.molpro.net}}, - Title = {MOLPRO, a package of ab initio programs}} - -@article{MomShi-JCP-87, - Author = {T. Momose and T. Shida}, - Journal = {J. Chem. Phys.}, - Pages = {2832}, - Volume = {87}, - Year = {1987}} - -@article{MorCepSen-PRL-95, - Author = {S. Moroni and D. M. Ceperley and G. Senatore}, - Journal = {Phys. Rev. Lett.}, - Pages = {689}, - Volume = {75}, - Year = {1995}} - -@article{MorCohYan-JCP-06a, - Author = {Paula Mori-S\'anchez and Aron J. Cohen and Weitao Yang}, - Journal = {J. Chem. Phys.}, - Pages = {091102}, - Volume = {124}, - Year = {2006}} - -@article{MorCohYan-JCP-06, - Author = {P. Mori-S{\'a}nchez and A. J. Cohen and W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {201102}, - Volume = {125}, - Year = {2006}} - -@article{MorCohYan-PRA-12, - Author = {P. Mori-S{\'a}nchez and A. J. Cohen and W. Yang}, - Journal = {Phys. Rev. A}, - Pages = {042507}, - Volume = {85}, - Year = {2012}} - -@article{MorCohYan-PRL-08, - Author = {Paula Mori-S\'anchez and Aron J. Cohen and Weitao Yang}, - Journal = {Phys. Rev. Lett.}, - Pages = {146401}, - Volume = {100}, - Year = {2008}} - -@article{MorCohYan-PRL-09, - Author = {Mori-S\'anchez, Paula and Cohen, Aron and Yang, Weitao}, - Journal = {Phys. Rev. Lett.}, - Pages = {066403}, - Title = {Discontinuous Nature of the Exchange-Correlation Functional in Strongly Correlated Systems}, - Volume = {102}, - Year = {2009}} - -@article{MorMcmClaKimScu-JCTC-12, - Author = {M. A. Morales and J. McMinis and B. K. Clark and J. Kim and G. E. Scuseria}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2181}, - Volume = {8}, - Year = {2012}} - -@article{Mor-PR-29, - Author = {P. M. Morse}, - Journal = {Phys. Rev.}, - Pages = {57}, - Volume = {34}, - Year = {1929}} - -@article{MorSen-PRB-91, - Author = {S. Moroni and G. Senatore}, - Journal = {Phys. Rev. B}, - Pages = {9864}, - Volume = {{44}}, - Year = {1991}} - -@article{MorWuYan-JCP-05, - Author = {P. Mori-S{\'a}nchez and Q. Wu and W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {062204}, - Volume = {123}, - Year = {2005}} - -@article{MosDep-JCTC-19, - Author = {{M. Mostafanejad and A. E. DePrince III}}, - Journal = {J. Chem. Theory Comput.}, - Pages = {290}, - Volume = {15}, - Year = {2019}} - -@article{MosJezSza-IJQC-93, - Author = {R. Moszynski and B. Jeziorski and K. Szalewicz}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {409}, - Volume = {45}, - Year = {1993}} - -@article{MosSan-IJQC-91, - Author = {F. Moscardo and E. San-Fabian}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {23}, - Volume = {{40}}, - Year = {1991}} - -@article{MosSan-PRA-91, - Author = {F. Moscard\'o and E. San-Fabi\'an}, - Journal = {Phys. Rev. A}, - Pages = {1549}, - Volume = {44}, - Year = {1991}} - -@article{MosSchLeeKal-JCP-82, - Author = {J. W. Moskowitz and K. E. Schmidt and M. A. Lee and M. H. Kalos}, - Journal = {J. Chem. Phys.}, - Pages = {349}, - Title = {{A new look at correlation energy in atomic and molecular systems. II. The application of the Green's function Monte Carlo method to LiH}}, - Volume = {77}, - Year = {1982}} - -@article{MosYabBon-TEC-66, - Author = {A. F. Moskvin and O. P. Yablonskii and L. F. Bondar}, - Journal = {Theor. Exp. Chem.}, - Pages = {636}, - Volume = {2}, - Year = {1966}} - -@article{MugPalNavEgu-PR-04, - Author = {J. G. Muga and J. P. Palao and B. Navarro and I. L. Egusquiza}, - Journal = {Phys. Rep.}, - Pages = {357}, - Volume = {395}, - Year = {2004}} - -@article{Mul-PLA-84, - Author = {A. M. K. M{\"u}ller}, - Journal = {Phys. Lett. A}, - Pages = {446}, - Volume = {105}, - Year = {1984}} - -@article{murray:7145, - Author = {Christopher W. Murray and Nicholas C. Handy and Roger D. Amos}, - Journal = {The Journal of Chemical Physics}, - Keywords = {OZONE; SULFUR; BERYLLIUM; HYDROCARBONS; PERTURBATION THEORY; DENSITY FUNCTIONAL METHOD; ACCURACY; DIMERS; GROUND STATES; PHYSICAL PROPERTIES}, - Number = {9}, - Pages = {7145-7151}, - Publisher = {AIP}, - Title = {A study of O[sub 3], S[sub 3], CH[sub 2], and Be[sub 2] using Kohn--Sham theory with accurate quadrature and large basis sets}, - Url = {http://link.aip.org/link/?JCP/98/7145/1}, - Volume = {98}, - Year = {1993}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/98/7145/1}} - -@article{MusAng-CTC-15, - Abstract = {Abstract The charge density response function and the exchange hole are closely related to each other via the fundamental fluctuation--dissipation theorem of physics. A simple approximate model of the static response function is visually compared on several examples in order to demonstrate this relationship. This study is completed by illustrating the well-known isomorphism between the exchange hole and the square of the dominant localized orbital lying in the space region of the reference point of the exchange hole function. The implications of these relationships for the interpretation of common chemical concepts, such as delocalization, are discussed. }, - Author = {Bastien Mussard and J\'anos G. \'Angy\'an}, - Doi = {http://dx.doi.org/10.1016/j.comptc.2014.10.039}, - Issn = {2210-271X}, - Journal = {Computational and Theoretical Chemistry}, - Keywords = {Topological analysis}, - Note = {Special Issue: Understanding structure and reactivity from topology and beyond}, - Number = {0}, - Pages = {44 - 52}, - Title = {Relationships between charge density response functions, exchange holes and localized orbitals}, - Url = {http://www.sciencedirect.com/science/article/pii/S2210271X14004952}, - Volume = {1053}, - Year = {2015}, - Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/pii/S2210271X14004952}, - Bdsk-Url-2 = {http://dx.doi.org/10.1016/j.comptc.2014.10.039}} - -@article{MusAng-TCA-15, - Author = {B. Mussard and J. G. \'Angy\'an}, - Doi = {http://dx.doi.org/10.1007/s00214-015-1751-2}, - Journal = {Theor. Chem. Acc.}, - Pages = {148}, - Volume = {134}, - Year = {2015}, - Bdsk-Url-1 = {http://dx.doi.org/10.1007/s00214-015-1751-2}} - -@incollection{MusCocAssOttUmrTou-AQC-18, - Author = {B. Mussard and E. Coccia and R. Assaraf and M. Otten and C. J. Umrigar and J. Toulouse}, - Booktitle = {Novel Electronic Structure Theory: General Innovations and Strongly Correlated Systems}, - Doi = {10.1016/bs.aiq.2017.05.005}, - Editor = {P. E. Hoggan}, - Pages = {255-270}, - Publisher = {Academic Press}, - Series = {Advances in Quantum Chemistry Vol. 76}, - Title = {Time-dependent linear-response variational Monte Carlo}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1016/bs.aiq.2017.05.005}} - -@article{MusReiAngTou-JCP-15, - Author = {B. Mussard and P. Reinhardt and J. G. \'Angy\'an and J. Toulouse}, - Journal = {J. Chem. Phys.}, - Note = {Erratum: J. Chem. Phys. {\bf 142}, 219901 (2015)}, - Pages = {154123}, - Title = {Spin-unrestricted random-phase approximation with range separation: Benchmark on atomization energies and reaction barrier heights}, - Volume = {142}, - Year = {2015}} - -@misc{MusReiAngTou-JJJ-XX-note, - Note = {See the supplementary material for the detailed results of the calculations on the AE49 and DBH24/08 datasets.}} - -@article{MusRocJanAng-JCTC-16, - Author = {B. Mussard and D. Rocca and G. Jansen and J. G. \'Angy\'an}, - Doi = {10.1021/acs.jctc.5b01129}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2191-2202}, - Title = {Dielectric Matrix Formulation of Correlation Energies in the Random Phase Approximation: Inclusion of Exchange Effects}, - Volume = {12}, - Year = {2016}, - Bdsk-Url-1 = {https://doi.org/10.1021/acs.jctc.5b01129}} - -@article{MusRocJanAng-JJJ-XX, - Author = {B. Mussard and D. Rocca and G. Jansen and J. G. \'Angy\'an}, - Note = {unpublished}} - -@article{MusSzaAng-JCTC-14, - Author = {B. Mussard and P. G. Szalay and J. G. \'Angy\'an}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1968}, - Volume = {10}, - Year = {2014}} - -@misc{MusTou-JJJ-XX, - Author = {B. Mussard and J. Toulouse}, - Note = {Fractional-charge and fractional-spin errors in range-separated density-functional theory, Mol. Phys., to appear (2016); preprint arXiv:1607.03621}} - -@article{MusTou-MP-17, - Author = {Bastien Mussard and Julien Toulouse}, - Journal = {Mol. Phys.}, - Pages = {161-173}, - Title = {Fractional-charge and fractional-spin errors in range-separated density-functional theory}, - Volume = {115}, - Year = {2017}} - -@article{Nag-IJQC-04, - Author = {A. Nagy}, - Journal = {Int. J. Quantum Chem.}, - Pages = {256}, - Volume = {99}, - Year = {2004}} - -@article{Nag-IJQC-98, - Author = {A. Nagy}, - Journal = {Int. J. Quantum Chem.}, - Pages = {681}, - Volume = {70}, - Year = {1998}} - -@article{Nag-JCP-06, - Author = {\'A. Nagy}, - Journal = {J. Chem. Phys.}, - Pages = {184104}, - Volume = {125}, - Year = {2006}} - -@article{NagLev-PRA-01, - Author = {A. Nagy and M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {052502}, - Volume = {63}, - Year = {2001}} - -@article{nagy:134107, - Author = {A. Nagy and S. Liu and L. Bartolloti}, - Eid = {134107}, - Journal = {The Journal of Chemical Physics}, - Keywords = {density functional theory; potential energy functions}, - Number = {13}, - Numpages = {5}, - Pages = {134107}, - Publisher = {AIP}, - Title = {Generalized density functional theory for degenerate states}, - Url = {http://link.aip.org/link/?JCP/122/134107/1}, - Volume = {122}, - Year = {2005}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/122/134107/1}} - -@article{NalPar-JCP-82, - Author = {Roman F. Nalewajski and Robert G. Parr}, - Journal = {J. Chem. Phys.}, - Note = {[In Eq.~(70) of this paper the minimization over potentials should actually be a maximization.]}, - Pages = {399-407}, - Publisher = {AIP}, - Title = {Legendre transforms and Maxwell relations in density functional theory}, - Volume = {77}, - Year = {1982}} - -@article{NalPar-JCP-fr-82, - Author = {Roman F. Nalewajski and Robert G. Parr}, - Journal = {J. Chem. Phys.}, - Note = {[Dans l'\'equation~(70) de cet article la minimisation sur le potentiel est en r\'ealit\'e une maximisation.]}, - Pages = {399-407}, - Publisher = {AIP}, - Title = {Legendre transforms and Maxwell relations in density functional theory}, - Volume = {77}, - Year = {1982}} - -@article{NeeSchKosSchGri-JCTC-09, - Author = {F. Neese and T. Schwabe and S. Kossmann and B. Schirmer and S. Grimme}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3060}, - Volume = {5}, - Year = {2009}} - -@article{NemTowNee-JCP-10, - Author = {N. Nemec and M. D. Towler and R. J. Needs}, - Journal = {J. Chem. Phys.}, - Pages = {034111}, - Volume = {132}, - Year = {2010}} - -@article{NesPey-JPB-90, - Author = {B. M. Nestmann and S. D. Peyerimhoff}, - Journal = {J. Phys. B}, - Pages = {L773}, - Volume = {23}, - Year = {1990}} - -@article{NeuBae-JCP-89a, - Author = {D. Neuhasuer and M. Baer}, - Journal = {J. Chem. Phys.}, - Pages = {4351}, - Volume = {90}, - Year = {1989}} - -@article{NeuHan-CPL-96, - Author = {R. Neumann and N. C. Handy}, - Journal = {Chem. Phys. Lett.}, - Pages = {19}, - Volume = {252}, - Year = {1996}} - -@article{NeuNobHan-MP-96, - Author = {R. Neumann and R. H. Nobes and N. C. Handy}, - Journal = {Mol. Phys.}, - Pages = {1}, - Volume = {87}, - Year = {1996}} - -@article{NguDayPac-JCP-11, - Author = {K. A. Nguyen and P. N. Day and R. Pachter}, - Journal = {J. Chem. Phys.}, - Pages = {074109}, - Volume = {135}, - Year = {2011}} - -@article{NguGal-JCP-10, - Author = {Huy-Viet Nguyen and Giulia Galli}, - Journal = {J. Chem. Phys.}, - Pages = {044109}, - Volume = {132}, - Year = {2010}} - -@article{NguGir-PRB-09, - Author = {Huy-Viet Nguyen and Stefano de Gironcoli}, - Journal = {Phys. Rev. B.}, - Pages = {205114}, - Volume = {79}, - Year = {2009}} - -@book{Nie-BOOK-92, - Author = {Harald Niederreiter}, - Publisher = {Society for Industrial and Applied Mathematics}, - Title = {Random Number Generation and Quasi-Monte Carlo Methods}, - Year = {1992}} - -@article{NieJorOdd-JCP-80, - Author = {E. S. Nielsen and P. J{\o}rgensen and J. Oddershede}, - Journal = {J. Chem. Phys.}, - Pages = {6238}, - Volume = {73}, - Year = {1980}} - -@article{NigBlo-PRB-86, - Author = {M. P. Nightingale and H. W. J. Bl\"ote}, - Journal = {Phys. Rev. B}, - Pages = {659}, - Title = {{Gap of the linear spin-1 Heisenberg antiferromagnet: A Monte Carlo calculation}}, - Volume = {33}, - Year = {1986}} - -@article{NigBlo-PRL-88, - Author = {M. P. Nightingale and H. Blote}, - Journal = {Phys. Rev. Lett.}, - Pages = {1562}, - Volume = {60}, - Year = {1988}} - -@article{NigMel-PRL-01, - Author = {M. P. Nightingale and V. Melik-Alaverdian}, - Journal = {Phys. Rev. Lett.}, - Pages = {043401}, - Title = {{Optimization of ground- and excited-state wave functions and van der Waals clusters}}, - Volume = {87}, - Year = {2001}} - -@book{NigUmr-BOOK-99, - Address = {Dordrecht}, - Editor = {M. P. Nightingale and C. J. Umrigar}, - Publisher = {Kluwer}, - Series = {NATO ASI Ser. C 525}, - Title = {Quantum Monte Carlo Methods in Physics and Chemistry}, - Year = {1999}} - -@incollection{NigUmr-INC-98, - Address = {NY}, - Author = {M. P. Nightingale and C. J. Umrigar}, - Booktitle = {Monte Carlo Methods in Chemistry}, - Editor = {D. M. Ferguson and J. I. Siepmann and D. G. Truhlar}, - Pages = {Chapter 4}, - Publisher = {Wiley}, - Series = {Advances in Chemical Physics Vol. 105}, - Year = {1998}} - -@article{Nik-PRB-74, - Author = {G. Niklasson}, - Journal = {Phys. Rev. B.}, - Pages = {3052}, - Volume = {{10}}, - Year = {1974}} - -@article{NiqFucGon-JCP-03, - Author = {Y. M. Niquet and M. Fuchs and X. Gonze}, - Journal = {J. Chem. Phys.}, - Pages = {9504}, - Volume = {118}, - Year = {2003}} - -@article{NiqFucGon-PRL-03, - Author = {Y. M. Niquet and M. Fuchs and X. Gonze}, - Journal = {Phys. Rev. Lett.}, - Pages = {219301}, - Volume = {90}, - Year = {2003}} - -@article{NiqGon-PRB-04, - Author = {Y. M. Niquet and X. Gonze}, - Journal = {Phys. Rev. B}, - Pages = {245115}, - Volume = {70}, - Year = {2004}} - -@misc{Nis-BOOK-05, - Title = {NIST Chemistry WebBook, NIST Standard Reference Database Number 69, June 2005 Release}, - Url = {http://webbook.nist.gov/chemistry York}, - Bdsk-Url-1 = {http://webbook.nist.gov/chemistry%20York}} - -@book{NIST-BOOK-05, - Address = {Gaithersburg}, - Editor = {P. J. Linstrom and W. G. Mallard}, - Publisher = {NIST}, - Title = {NIST Chemistry WebBook, NIST Standard Reference Database Number 69}, - Year = {June 2005}} - -@misc{NIST-BOOK-15, - Author = {{NIST Computational Chemistry Comparison and Benchmark Database}}, - Editor = {{Russell D. Johnson III}}, - Title = {{NIST Standard Reference Database Number 101, Release 17b}}, - Url = {http://cccbdb.nist.gov/}, - Year = {September 2015}, - Bdsk-Url-1 = {http://cccbdb.nist.gov/}} - -@article{NogHiyAkiKog-JCP-14, - Author = {Y. Noguchi and M. Hiyama and H. Akiyama and N. Koga}, - Journal = {J. Chem. Phys.}, - Pages = {044309}, - Volume = {141}, - Year = {2014}} - -@article{NooShaMuk-MP-05, - Author = {M. Nooijen and K. R. Shamasundary and D. Mukherjee}, - Journal = {Mol. Phys.}, - Pages = {2277}, - Volume = {103}, - Year = {2005}} - -@article{NorJieSer-JCP-03, - Author = {P. Norman and A. Jiemchooroj and Bo E. Sernelius}, - Journal = {J. Chem. Phys.}, - Pages = {9167}, - Volume = {118}, - Year = {2003}} - -@article{NozPin-PR-58, - Author = {P. Nozi\`eres and D. Pines}, - Journal = {Phys. Rev.}, - Pages = {442}, - Volume = {111}, - Year = {1958}} - -@article{Odd-AQC-78, - Author = {Jens Oddershede}, - Journal = {Adv. Quantum Chem.}, - Pages = {275}, - Title = {Polarization Propagator Calculations}, - Volume = {11}, - Year = {1978}} - -@article{OddJor-JCP-77, - Author = {J. Oddershede and P. J{\o}rgensen}, - Journal = {J. Chem. Phys.}, - Pages = {1541}, - Volume = {66}, - Year = {1977}} - -@article{OlePalOniDel-PRB-99, - Author = {Valerio Olevano and Maurizia Palummo and Giovanni Onida and Rodolfo Del Sole}, - Journal = {Phys. Rev. B}, - Pages = {14224}, - Volume = {{60}}, - Year = {1999}} - -@article{OleTouSch-JCP-19, - Author = {Valerio Olevano and Julien Toulouse and Peter Schuck}, - Doi = {10.1063/1.5080330}, - Journal = {J. Chem. Phys.}, - Pages = {084112}, - Title = {A formally exact one-frequency-only Bethe-Salpeter-like equation. Similarities and differences between GW+BSE and self-consistent RPA}, - Volume = {150}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5080330}} - -@article{OliBotMar-PCCP-11, - Author = {M. J. T. Oliveira and S. Botti and M. A. L. Marques}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {15055}, - Volume = {13}, - Year = {2011}} - -@article{OliPer-PRA-79, - Author = {G. L. Oliver and J. P. Perdew}, - Journal = {Phys. Rev. A}, - Pages = {397}, - Volume = {20}, - Year = {1979}} - -@article{OniReiRub-RMP-02, - Author = {G. Onida and L. Reining and A. Rubio}, - Journal = {Rev. Mod. Phys.}, - Pages = {601}, - Title = {{Electronic excitations: density-functional versus many-body Green's-function approaches}}, - Volume = {74}, - Year = {2002}} - -@article{OrtBal-PRB-94, - Author = {G. Ortiz and P. Ballone}, - Journal = {Phys. Rev. B}, - Pages = {1391}, - Volume = {{50}}, - Year = {1994}} - -@article{OrtBal-PRB-err-97, - Author = {G. Ortiz and P. Ballone}, - Journal = {Phys. Rev. B}, - Pages = {9970}, - Volume = {{56}}, - Year = {1997}} - -@misc{Ort-PROG-XX, - Author = {P. Reinhardt}, - Note = {Different programs to perform ab-initio calculations within highly localized orbitals (Toulouse-Dresden-Paris, 1998--), unpublished}} - -@article{OsiGisSniBae-JCP-97, - Author = {{V. P. Osinga, S. J. A. van Gisbergen, J. G. Snijders, and E. J. Baerends}}, - Journal = {J. Chem. Phys.}, - Pages = {5091}, - Volume = {106}, - Year = {1997}} - -@article{OstKar-CPL-71, - Author = {N. Ostlund and M. Karplus}, - Journal = {Chem. Phys. Lett.}, - Pages = {450}, - Volume = {11}, - Year = {1971}} - -@misc{OthMonMar-ARX-16, - Author = {{A. A. Othman, M. de Montigny, and F. Marsiglio}}, - Note = {\url{http://arxiv.org/abs/1612.06706}}, - Title = {The Coulomb potential in quantum mechanics revisited}} - -@article{Ove-CJP-95, - Author = {A. W. Overhauser}, - Journal = {Can. J. Phys.}, - Pages = {683}, - Volume = {{73}}, - Year = {1995}} - -@article{PacBye-JCP-66, - Author = {{R. T. Pack and W. Byers-Brown}}, - Journal = {J. Chem. Phys.}, - Pages = {556}, - Title = {{Cusp conditions for molecular wavefunctions}}, - Volume = {45}, - Year = {1966}} - -@article{PaiJanHenScuGruKre-JCP-10, - Author = {J. Paier and B. G. Janesko and T. M. Henderson and G. E. Scuseria and A. Gr\"uneis and G. Kresse}, - Journal = {J. Chem. Phys.}, - Pages = {094103}, - Volume = {132}, - Year = {2010}} - -@article{PaiMarHumKreGerAng-JCP-06, - Author = {J. Paier and M. Marsman and K. Hummer and G. Kresse and I. C. Gerber and J. G. \'Angy\'an}, - Journal = {J. Chem. Phys.}, - Pages = {154709}, - Volume = {124}, - Year = {2006}} - -@article{PaiMarKre-JCP-07, - Author = {Joachim Paier and Martijn Marsman and Georg Kresse}, - Doi = {10.1063/1.2747249}, - Eid = {024103}, - Journal = {The Journal of Chemical Physics}, - Keywords = {HF calculations; density functional theory; heat of formation; lattice constants; electron gas; electron correlations; elastic moduli}, - Number = {2}, - Numpages = {10}, - Pages = {024103}, - Publisher = {AIP}, - Title = {Why does the B3LYP hybrid functional fail for metals?}, - Url = {http://link.aip.org/link/?JCP/127/024103/1}, - Volume = {127}, - Year = {2007}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/127/024103/1}, - Bdsk-Url-2 = {https://doi.org/10.1063/1.2747249}} - -@article{PaiRenRinScuGruKreSch-NJP-12, - Author = {Joachim Paier and Xinguo Ren and Patrick Rinke and Gustavo E. Scuseria and Andreas Gr\"uneis and Georg Kresse and Matthias Scheffler}, - Journal = {New J. Phys.}, - Pages = {043002}, - Volume = {14}, - Year = {2012}} - -@article{PalCiz-JCP-70, - Author = {J. Paldus and J. {\v C}i{\v z}ek}, - Journal = {J. Chem. Phys.}, - Pages = {2919}, - Volume = {52}, - Year = {1970}} - -@article{PalCis-JCP-71, - Author = {J. Paldus and J. {\v C}i{\v z}ek}, - Journal = {J. Chem. Phys.}, - Pages = {2293}, - Volume = {54}, - Year = {1971}} - -@article{PalCiz-PRA-70, - Author = {J. Paldus and J. {\v C}i{\v z}ek}, - Journal = {Phys. Rev. A}, - Pages = {2268}, - Volume = {2}, - Year = {1970}} - -@article{Pal-JCP-77, - Author = {J. Paldus}, - Journal = {J. Chem. Phys.}, - Pages = {303}, - Volume = {67}, - Year = {1977}} - -@article{PalOniDelCorRei-PRB-99, - Author = {Maurizia Palummo and Giovanni Onida and Rodolfo Del Sole and Massimiliano Corradini and Lucia Reining}, - Journal = {Phys. Rev. B}, - Pages = {11329}, - Volume = {{60}}, - Year = {1999}} - -@article{PalPavHubSch-EPJB-11, - Author = {G. Pal and Y. Pavlyukh and W. H\"ubner and H. C. Schneider}, - Journal = {Eur. Phys. J. B.}, - Pages = {327}, - Volume = {79}, - Year = {2011}} - -@article{Pan-CPL-93, - Author = {I. Panas}, - Journal = {Chem. Phys. Lett.}, - Pages = {255}, - Volume = {201}, - Year = {1993}} - -@article{pan:5642, - Author = {Xiao-Yin Pan and Viraht Sahni}, - Issue = {12}, - Journal = {The Journal of Chemical Physics}, - Keywords = {ground states; molecular configurations; density functional theory; Schrodinger equation; ionisation potential; wave functions; eigenvalues and eigenfunctions; electron correlations; hydrogen}, - Page = {5642-5649}, - Publisher = {AIP}, - Title = {Quantal density functional theory of the hydrogen molecule}, - Url = {http://link.aip.org/link/?JCP/120/5642/1}, - Volume = {120}, - Year = {2004}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/120/5642/1}} - -@article{PaqTou-JCP-18, - Author = {Julien Paquier and Julien Toulouse}, - Doi = {10.1063/1.5049773}, - Journal = {J. Chem. Phys.}, - Pages = {174110}, - Title = {Four-component relativistic range-separated density-functional theory: Short-range exchange local-density approximation}, - Volume = {149}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5049773}} - -@misc{PaqTou-JJJ-XX-note, - Note = {See Supplementary Information for details on the calculation of the sums over spins in Eqs.~(\ref{epsxC}) and (\ref{epsxB}), details on the calculation of the large-$\ct$ expansions in Eqs.~(\ref{epsCsrasymp}) and~(\ref{epsBsrasymp}), and for a Mathematica notebook containing the complete expressions of the large-$\ct$ expansions in Eqs.~(\ref{epsCsrasymp}) and~(\ref{epsBsrasymp}) and of the Pad\'e approximants in Eqs.~(\ref{PadeC}) and~(\ref{PadeB}).}} - -@article{parr:3801, - Author = {Robert G. Parr and Robert A. Donnelly and Mel Levy and William E. Palke}, - Journal = {The Journal of Chemical Physics}, - Number = {8}, - Pages = {3801-3807}, - Publisher = {AIP}, - Title = {Electronegativity: The density functional viewpoint}, - Url = {http://link.aip.org/link/?JCP/68/3801/1}, - Volume = {68}, - Year = {1978}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/68/3801/1}} - -@book{ParYan-BOOK-89, - Address = {New York}, - Author = {R. G. Parr and W. Yang}, - Publisher = {Oxford University Press}, - Title = {Density-Functional Theory of Atoms and Molecules}, - Year = {1989}} - -@article{PasGidPer-PRA-13, - Author = {E. Pastorczak and N. I. Gidopoulos and K. Pernal}, - Journal = {Phys. Rev. A}, - Pages = {062501}, - Volume = {87}, - Year = {2013}} - -@article{PatCenJezJezSza-JPCA-07, - Author = {Konrad Patkowski and Wojciech Cencek and M. Jeziorska and B. Jeziorski and Krzysztof Szalewicz}, - Journal = {J. Phys. Chem. A}, - Pages = {7611}, - Volume = {111}, - Year = {2007}} - -@article{PatVas-PRB-72, - Author = {K. N. Pathak and P. Vashishta}, - Journal = {Phys. Rev. B.}, - Pages = {3649}, - Volume = {{7}}, - Year = {1972}} - -@book{Pauncz-BOOK-79, - Address = {New York}, - Author = {R. Pauncz}, - Publisher = {Plenum Press}, - Title = {Spin Eigenfunctions}, - Year = {1979}} - -@article{PauPilTouEll-JCP-10, - Author = {Fran\c{c}oise Pauzat and Julien Pilm\'e and Julien Toulouse and Yves Ellinger}, - Journal = {J. Chem. Phys.}, - Pages = {054301}, - Title = {About the collapse of the 3.3 µm CH stretching band with ionization in polycyclic aromatic hydrocarbons: Configuration interaction and quantum Monte Carlo studies of the CH fragment}, - Volume = {133}, - Year = {2010}} - -@article{PazMorGorBac-PRB-06, - Author = {Simone Paziani and Saverio Moroni and Paola Gori-Giorgi and Giovanni B. Bachelet}, - Journal = {Phys. Rev. B}, - Pages = {155111}, - Volume = {73}, - Year = {2006}} - -@article{PazMorGorBac-xxx-xx, - Author = {S. Paziani and S. Moroni and P. Gori-Giorgi and G. B. Bachelet}, - Journal = {in preparation}, - Volume = {{}}, - Year = {2005}} - -@article{PeaBenHelToz-JCP-08, - Author = {M. J. Peach and P. Benfield and T. Helgaker and D. J. Tozer}, - Journal = {J. Chem. Phys.}, - Pages = {044118}, - Volume = {128}, - Year = {2008}} - -@article{PeaCohToz-PCCP-06, - Author = {M. J. G. Peach and A. J. Cohen and D. J. Tozer}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {4543}, - Volume = {8}, - Year = {2006}} - -@article{PeaHelSalKeaLutTozHan-PCCP-06, - Author = {M. J. G. Peach and T. Helgaker and P. Salek and T. W. Keal and O. B. Lutn{\ae}s and D. J. Tozer and N. C. Handy}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {558}, - Volume = {8}, - Year = {2006}} - -@article{PeaTeaHelToz-JCTC-15, - Author = {M. J. G. Peach and A. M. Teale and T. Helgaker and D. J. Tozer}, - Journal = {J. Chem. Theory Comput.}, - Pages = {5262}, - Volume = {11}, - Year = {2015}} - -@article{PeaToz-JPCA-12, - Author = {M. J. G. Peach and D. J. Tozer}, - Journal = {J. Phys. Chem. A}, - Pages = {9783}, - Volume = {116}, - Year = {2012}} - -@misc{PedJen-JJJ-XX, - Author = {J. K. Pedersen and H. J. A. Jensen}, - Note = {(unpublished)}, - Title = {{A second order MCSCF-DFT hybrid algorithm}}} - -@misc{PedJen-JJJ-XX_fr, - Author = {J. K. Pedersen and H. J. A. Jensen}, - Note = {non publi{\'e}}} - -@phdthesis{Ped-THESIS-04, - Address = {Odense}, - Author = {J. K. Pedersen}, - School = {University of Southern Denmark}, - Title = {Description of correlation and relativistic effects in calculations of molecular properties}, - Type = {{PhD thesis}}, - Year = {2004}} - -@article{PeiNecWar-PRA-03, - Author = {K. Peirs and D. Van Neck and M. Waroquier}, - Eid = {012505}, - Issue = {1}, - Journal = {Physical Review A (Atomic, Molecular, and Optical Physics)}, - Keywords = {density functional theory; atomic structure; Green's function methods; ab initio calculations}, - Numpages = {12}, - Page = {012505}, - Publisher = {APS}, - Title = {Algorithm to derive exact exchange-correlation potentials from correlated densities in atoms}, - Url = {http://link.aps.org/abstract/PRA/v67/e012505}, - Volume = {67}, - Year = {2003}, - Bdsk-Url-1 = {http://link.aps.org/abstract/PRA/v67/e012505}} - -@article{PerBurErn-PRL-96, - Author = {J. P. Perdew and K. Burke and M. Ernzerhof}, - Journal = {Phys. Rev. Lett.}, - Pages = {3865}, - Title = {Generalized Gradient Approximation Made Simple}, - Volume = {77}, - Year = {1996}} - -@article{PerCheVosJacPedSinFio-PRB-92, - Author = {J. P. Perdew and J. A. Chevary and S. H. Vosko and K. A. Jackson and M. R. Pederson and D. J. Singh and C. Fiolhais}, - Journal = {Phys. Rev. B}, - Pages = {6671}, - Volume = {{46}}, - Year = {1992}} - -@book{PerEngDreGroGodNogCasMar-BOOK-03, - Address = {Berlin}, - Editor = {C. Fiolhais and F. Nogueira and M. A. L. Marques}, - Publisher = {Springer}, - Series = {Vol. 620 of Lecture Notes in Physics}, - Title = {A Primer in Density Functional Theory}, - Year = {2003}} - -@article{PerErnBur-JCP-96, - Author = {J. P. Perdew and M. Ernzerhof and K. Burke}, - Journal = {J. Chem. Phys}, - Pages = {9982}, - Volume = {105}, - Year = {1996}} - -@article{PerErnBurSav-IJQC-97, - Author = {J. P. Perdew and M. Ernzerhof and K. Burke and A. Savin}, - Journal = {Int. J. Quantum Chem.}, - Pages = {197}, - Volume = {{61}}, - Year = {1997}} - -@article{PerGieGriBae-JCP-07, - Author = {K. Pernal and K. Giesbertz and O. Gritsenko and E. J. Baerends}, - Journal = {J. Chem. Phys.}, - Pages = {214101}, - Volume = {127}, - Year = {2007}} - -@article{PerGriBae-PRA-07, - Author = {K. Pernal and O. Gritsenko and E. J. Baerends}, - Journal = {Phys. Rev. A}, - Pages = {012506}, - Volume = {75}, - Year = {2007}} - -@article{PerGriMee-JCP-19, - Author = {{K. Pernal, O. V. Gritsenko, and R. van Meer}}, - Journal = {J. Chem. Phys.}, - Pages = {164122}, - Volume = {151}, - Year = {2019}} - -@article{Per-IJQC-93, - Author = {J. P. Perdew}, - Journal = {Int. J. Quantum. Chem.: Quantum Chem. Symp.}, - Pages = {93}, - Volume = {27}, - Year = {1993}} - -@incollection{Per-INC-91, - Address = {berlin}, - Author = {J. P. Perdew}, - Booktitle = {Electronic Structure of Solids '91}, - Editor = {P. Ziesche and H. Eschrig}, - Publisher = {Akademie Verlag}, - Year = {1991}} - -@article{Per-JCP-12, - Author = {K. Pernal}, - Journal = {J. Chem. Phys.}, - Pages = {184105}, - Title = {{Excitation energies from range-separated time-dependent density and density matrix functional theory}}, - Volume = {136}, - Year = {2012}} - -@article{PerLanSah-PRL-77, - Author = {J. P. Perdew and D. C. Langreth and V. Sahni}, - Journal = {Phys. Rev. Lett.}, - Pages = {1030}, - Volume = {{38}}, - Year = {1977}} - -@article{PerLev-PRL-83, - Author = {J. P. Perdew and M. Levy}, - Journal = {Phys. Rev. Lett.}, - Pages = {1884}, - Volume = {51}, - Year = {1983}} - -@article{PerMcMZun-PRA-81, - Author = {J. P. Perdew and E. R. McMullen and A. Zunger}, - Journal = {Phys. Rev. A}, - Pages = {2785}, - Volume = {{23}}, - Year = {1981}} - -@article{PerParLevBal-PRL-82, - Author = {J. P. Perdew and R. G. Parr and M. Levy and J. L. Balduz}, - Journal = {Phys. Rev. Lett.}, - Pages = {1691}, - Title = {Density-functional theory for fractional particle number: Derivative discontinuity of the energy}, - Volume = {49}, - Year = {1982}} - -@article{PerPerMorIll-JCC-07, - Author = {A. J. P\'erez-Jim\'enez and J. M. P\'erez-Jord\'a and I. De P. R. Moreira and F. Illas}, - Journal = {J. Comput. Chem.}, - Pages = {2559}, - Volume = {28}, - Year = {2007}} - -@article{PerPerSan-JCP-07, - Author = {A. J. P\'erez-Jim\'enez and J. M. P\'erez-Jord\'a and J. C. Sancho-Garc\'ia}, - Journal = {J. Chem. Phys.}, - Pages = {104102}, - Title = {Combining two-body density correlation functionals with multiconfigurational wave functions using natural orbitals and occupation numbers}, - Volume = {127}, - Year = {2007}} - -@article{Per-PRA-10, - Author = {Katarzyna Pernal}, - Journal = {Phys. Rev. A}, - Pages = {052511}, - Volume = {81}, - Year = {2010}} - -@article{Per-PRB-86, - Author = {J. P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {8822}, - Volume = {{33}}, - Year = {1986}} - -@article{Per-PRL-85, - Author = {J. P. Perdew}, - Journal = {Phys. Rev. Lett.}, - Pages = {1665}, - Volume = {{55}}, - Year = {1985}} - -@article{PerSavBur-PRA-95, - Author = {J. P. Perdew and A. Savin and K. Burke}, - Journal = {Phys. Rev. A}, - Pages = {4531}, - Title = {{Escaping the symmetry dilemma through a pair-density interpretation of spin-density functional theory}}, - Volume = {51}, - Year = {1995}} - -@article{PerSunRuzMezCso-PPCE-16, - Author = {J. P. Perdew and J. Sun and A. Ruzsinszky and P. D. Mezei and G. I. Csonka}, - Journal = {Period. Polytech. Chem. Eng.}, - Pages = {2}, - Volume = {60}, - Year = {2016}} - -@article{PerWan2-PRB-92, - Author = {J. P. Perdew and Y. Wang}, - Journal = {Phys. Rev. B}, - Pages = {12947}, - Volume = {{46}}, - Year = {1992}} - -@article{PerWan-PRB-86, - Author = {J. P. Perdew and Y. Wang}, - Journal = {Phys. Rev. B}, - Pages = {8800}, - Volume = {{33}}, - Year = {1986}} - -@article{PerWan-PRB-92, - Author = {J. P. Perdew and Y. Wang}, - Journal = {Phys. Rev. B}, - Pages = {13244}, - Volume = {45}, - Year = {1992}} - -@article{PerZun-PRB-81, - Author = {J. P. Perdew and A. Zunger}, - Journal = {Phys. Rev. B}, - Pages = {5048}, - Volume = {23}, - Year = {1981}} - -@article{PetDun-JCP-02, - Author = {{K. A. Peterson and T. H. Dunning, Jr}}, - Journal = {J. Chem. Phys.}, - Pages = {10548}, - Volume = {117}, - Year = {2002}} - -@article{PetDun-JPC-95, - Author = {{K. A. Peterson and T. H. Dunning Jr.}}, - Journal = {J. Phys. Chem.}, - Pages = {3898}, - Volume = {99}, - Year = {1995}} - -@article{PetGosGro-PRL-96, - Author = {M. Petersilka and U. J. Gossmann and E. K. U. Gross}, - Journal = {Phys. Rev. Lett.}, - Pages = {1212}, - Volume = {76}, - Year = {1996}} - -@article{PetGro-IJQC-96, - Author = {M. Petersilka and E. K. U. Gross}, - Journal = {Int. J. Quantum Chem. Symp.}, - Pages = {1393}, - Volume = {30}, - Year = {1996}} - -@article{PetHolChaNigUmr-PRL-12, - Author = {F. R. Petruzielo and A. A. Holmes and H. J. Changlani and M. P. Nightingale and C. J. Umrigar}, - Journal = {Phys. Rev. Lett.}, - Pages = {230201}, - Title = {Semistochastic Projector Monte Carlo Method}, - Volume = {109}, - Year = {2012}} - -@article{PetKenDun-JCP-93b, - Author = {{K. A. Peterson, R. A. Kendall and T. H. Dunning Jr.}}, - Journal = {J. Chem. Phys.}, - Pages = {9790}, - Volume = {99}, - Year = {1993}} - -@article{PetTouUmr-JCP-11, - Author = {F. R. Petruzielo and J. Toulouse and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {064104}, - Title = {Basis set construction for molecular electronic structure theory: Natural orbital and Gauss--Slater basis for smooth pseudopotentials}, - Volume = {134}, - Year = {2011}} - -@article{PetTouUmr-JCP-12, - Author = {F. R. Petruzielo and J. Toulouse and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {124116}, - Title = {{Approaching chemical accuracy with quantum Monte Carlo}}, - Volume = {136}, - Year = {2012}} - -@article{PevHea-JCP-13, - Author = {Roberto Peverati and Martin Head-Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {024110}, - Title = {Orbital optimized double-hybrid density functionals}, - Volume = {139}, - Year = {2013}} - -@article{PevTru-JPCL-11, - Author = {Roberto Peverati and Donald G. Truhlar}, - Journal = {J. Phys. Chem. Lett.}, - Pages = {2810}, - Volume = {2}, - Year = {2011}} - -@article{PevTru-JPCL-12, - Author = {Roberto Peverati and Donald G. Truhlar}, - Journal = {J. Phys. Chem. Lett.}, - Pages = {117}, - Volume = {3}, - Year = {2012}} - -@article{PevTru-PTRSA-14, - Abstract = {Kohn{\textendash}Sham density functional theory is in principle an exact formulation of quantum mechanical electronic structure theory, but in practice we have to rely on approximate exchange{\textendash}correlation (xc) functionals. The objective of our work has been to design an xc functional with broad accuracy across as wide an expanse of chemistry and physics as possible, leading{\textemdash}as a long-range goal{\textemdash}to a functional with good accuracy for all problems, i.e. a universal functional. To guide our path towards that goal and to measure our progress, we have developed{\textemdash}building on earlier work of our group{\textemdash}a set of databases of reference data for a variety of energetic and structural properties in chemistry and physics. These databases include energies of molecular processes, such as atomization, complexation, proton addition and ionization; they also include molecular geometries and solid-state lattice constants, chemical reaction barrier heights, and cohesive energies and band gaps of solids. For this paper, we gather many of these databases into four comprehensive databases, two with 384 energetic data for chemistry and solid-state physics and another two with 68 structural data for chemistry and solid-state physics, and we test two wave function methods and 77 density functionals (12 Minnesota meta functionals and 65 others) in a consistent way across this same broad set of data. We especially highlight the Minnesota density functionals, but the results have broader implications in that one may see the successes and failures of many kinds of density functionals when they are all applied to the same data. Therefore, the results provide a status report on the quest for a universal functional.}, - Author = {Peverati, Roberto and Truhlar, Donald G.}, - Doi = {10.1098/rsta.2012.0476}, - Isbn = {1471-2962}, - Issn = {1364-503X}, - Journal = {Phil. Trans. R. Soc. A}, - Note = {preprint at http://arxiv.org/abs/1212.0944}, - Number = {2011}, - Pages = {20120476}, - Publisher = {The Royal Society}, - Title = {Quest for a universal density functional: the accuracy of density functionals across a broad spectrum of databases in chemistry and physics}, - Volume = {372}, - Year = {2014}, - Bdsk-Url-1 = {https://doi.org/10.1098/rsta.2012.0476}} - -@article{PhiKanZgi-JCP-15, - Author = {J. J. Phillips and A. A. Kananenka and D. Zgid}, - Journal = {J. Chem. Phys.}, - Pages = {194108}, - Volume = {142}, - Year = {2015}} - -@article{PicGos-MP-73, - Author = {B. T. Pickup and O. Goscinski}, - Journal = {Mol. Phys.}, - Pages = {1013}, - Volume = {26}, - Year = {1973}} - -@book{PinNoz-BOOK-89, - Author = {D. Pines and P. Nozi\`eres}, - Publisher = {Addison-Wesley Publishing Company}, - Title = {The Theory of Quantum Liquids}, - Year = {1989}} - -@article{PisDov-IJQC-80, - Author = {C. Pisani and R. Dovesi}, - Journal = {Int. J. Quantum Chem.}, - Pages = {501}, - Volume = {17}, - Year = {1980}} - -@article{PisMasCasHalSchUsv-JCC-08, - Author = {C. Pisani and L. Maschio and S. Casassa and M. Halo and M. Sch\"utz and D. Usvyat}, - Journal = {J. Comput. Chem.}, - Pages = {2113}, - Volume = {29}, - Year = {2008}} - -@article{pittner:10275, - Author = {Jiri Pittner and Petr Nachtigall and Petr Carsky and Jozef Masik and Ivan Hubac}, - Journal = {The Journal of Chemical Physics}, - Keywords = {organic compounds; silicon compounds; coupled cluster calculations; configuration interactions}, - Number = {21}, - Pages = {10275-10282}, - Publisher = {AIP}, - Title = {Assessment of the single-root multireference Brillouin--Wigner coupled- cluster method: Test calculations on CH[sub 2], SiH[sub 2], and twisted ethylene}, - Url = {http://link.aip.org/link/?JCP/110/10275/1}, - Volume = {110}, - Year = {1999}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/110/10275/1}} - -@article{PolColLeiStoWerSav-IJQC-03, - Author = {R. Pollet and F. Colonna and T. Leininger and H. Stoll and H.-J. Werner and A. Savin}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {84}, - Title = {Exchange-Correlation Energies and Correlation Holes for Some Two- and Four-Electron Atoms along a Nonlinear Adiabatic Connection in Density Functional Theory}, - Volume = {{91}}, - Year = {2003}} - -@article{PolSavLeiSto-JCP-02, - Author = {R. Pollet and A. Savin and T. Leininger and H. Stoll}, - Journal = {J. Chem. Phys.}, - Pages = {1250}, - Title = {Combining multideterminantal wave functions with density functionals to handle near-degeneracy in atoms and molecules}, - Volume = {{116}}, - Year = {2002}} - -@phdthesis{Pol-THESIS-01, - Author = {R. Pollet}, - School = {Universit\'e Paris 6}, - Title = {D\'eveloppement et applications d'une m\'ethode g\'en\'eralisant la th\'eorie de la fonctionnelle de la densit\'e \`a plusieurs d\'eterminants de Slater}, - Type = {Th\`ese de doctorat}, - Year = {2001}} - -@article{Pop-RMP-99, - Author = {J. A. Pople}, - Journal = {Rev. Mod. Phys.}, - Pages = {1267}, - Title = {{Nobel Lecture: Quantum chemical models}}, - Volume = {{71}}, - Year = {1999}} - -@article{PorDer-PRA-02, - Author = {S. G. Porsev and A. Derevianko}, - Journal = {Phys. Rev. A}, - Pages = {020701(R)}, - Volume = {65}, - Year = {2002}} - -@article{PraWooPetDunWil-TCA-11, - Author = {{B. P. Prascher, D. E. Woon, K. A. Peterson, T. H. Dunning, Jr., and A. K. Wilson}}, - Journal = {Theor. Chem. Acc.}, - Pages = {69}, - Volume = {128}, - Year = {2011}} - -@article{PreBevFah-PRB-02, - Author = {David Prendergast and David Bevan and Stephen Fahy}, - Journal = {Phys. Rev. B}, - Pages = {155104}, - Volume = {66}, - Year = {2002}} - -@article{PreNolFilFahGre-JCP-01, - Author = {D. Prendergast and M. Nolan and C. Filippi and S. Fahy and J. C. Greer}, - Journal = {J. Chem. Phys.}, - Pages = {1626}, - Volume = {{115}}, - Year = {2001}} - -@book{PreTeuVetFla-BOOK-92, - Address = {Cambridge}, - Author = {W. Press and S. Teukolsky and W. Vetterling and B. Flannery}, - Publisher = {Cambridge University Press}, - Title = {Numerical Recipes}, - Year = {1992}} - -@article{Pul-MP-69, - Author = {P. Pulay}, - Journal = {Mol. Phys.}, - Pages = {197}, - Volume = {17}, - Year = {1969}} - -@article{PurZhaKra-JCP-09, - Author = {W. Purwanto and S. Zhang and H. Krakauer}, - Journal = {J. Chem. Phys.}, - Pages = {094107}, - Volume = {130}, - Year = {2009}} - -@misc{Qmc-PROG-XX, - Note = {QMCMOL, a quantum Monte Carlo program written by R. Assaraf, F. Colonna, X. Krokidis, P. Reinhardt and coworkers.}, - Url = {http://www.lct.jussieu.fr/pagesequipe/qmcmol/qmcmol/}, - Bdsk-Url-1 = {http://www.lct.jussieu.fr/pagesequipe/qmcmol/qmcmol/}} - -@misc{Quantumexpressoweb-PROG-XX, - Note = {\url{http://www.quantum-espresso.org}}, - Title = {QUANTUM ESPRESSO, an integrated suite of Open-Source computer codes for electronic-structure calculations and materials modeling at the nanoscale}} - -@article{RabBaeNeu-PRB-15, - Author = {E. Rabani and R. Baer and D. Neuhauser}, - Journal = {Phys. Rev. B}, - Pages = {235302}, - Volume = {91}, - Year = {2015}} - -@article{rabinovitch:1807, - Author = {B. S. Rabinovitch and John E. Douglas and F. S. Looney}, - Journal = {The Journal of Chemical Physics}, - Number = {11}, - Pages = {1807-1808}, - Publisher = {AIP}, - Title = {The Thermal Trans-Cis Isomerization of Dideuteroethylene}, - Url = {http://link.aip.org/link/?JCP/20/1807/2}, - Volume = {20}, - Year = {1952}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/20/1807/2}} - -@book{Rai-BOOK-72, - Address = {Amsterdam-London}, - Author = {S. Raimes}, - Publisher = {North-Holland Publishing Company}, - Title = {Many-electron theory}, - Year = {1972}} - -@article{Raj-ACP-80, - Author = {A. K. Rajagopal}, - Journal = {Adv. Chem. Phys.}, - Pages = {59}, - Volume = {41}, - Year = {1980}} - -@article{RajCal-PRB-73, - Author = {A. K. Rajagopal and J. Callaway}, - Journal = {Phys. Rev. B}, - Pages = {1912}, - Volume = {7}, - Year = {1973}} - -@article{Raj-JPC-78, - Author = {A. K. Rajagopal}, - Journal = {J. Phys. C}, - Pages = {L943}, - Volume = {11}, - Year = {1978}} - -@article{RamLeoNeu-ARPC-16, - Author = {Krupa Ramasesha and Stephen R. Leone and Daniel M. Neumark}, - Journal = {Annu. Rev. Phys. Chem.}, - Pages = {41}, - Title = {Real-Time Probing of Electron Dynamics Using Attosecond Time-Resolved Spectroscopy}, - Volume = {67}, - Year = {2016}} - -@article{RamRaj-PRA-82, - Author = {M. V. Ramana and A. K. Rajagopal}, - Journal = {Phys. Rev. A}, - Pages = {96}, - Year = {1982}} - -@article{RasChi-JCP-96a, - Author = {V. A. Rassolov and D. M. Chipman}, - Journal = {J. Chem. Phys.}, - Pages = {1470}, - Volume = {105}, - Year = {1996}} - -@article{RasChi-JCP-96b, - Author = {V. A. Rassolov and D. M. Chipman}, - Journal = {J. Chem. Phys.}, - Pages = {1479}, - Volume = {105}, - Year = {1996}} - -@article{Rau-JAA-96, - Author = {A. R. P. Rau}, - Journal = {J. Astrophys. Astr.}, - Pages = {113}, - Volume = {17}, - Year = {1996}} - -@misc{RebSavTou-JJJ-XX, - Author = {E. Rebolini and A. Savin and J. Toulouse}, - Note = {unpublished}} - -@article{RebSavTou-MP-13, - Author = {E. Rebolini and A. Savin and J. Toulouse}, - Journal = {Mol. Phys.}, - Pages = {1219}, - Title = {Electronic excitations from a linear-response range-separated hybrid scheme}, - Volume = {111}, - Year = {2013}} - -@article{RebTeaHelSavTou-MP-18, - Author = {E. Rebolini and A. M. Teale and T. Helgaker and A. Savin and J. Toulouse}, - Doi = {doi.org/10.1080/00268976.2017.1422811}, - Journal = {Mol. Phys.}, - Pages = {1443-1451}, - Title = {Excitation energies from G\"orling--Levy perturbation theory along the range-separated adiabatic connection}, - Volume = {116}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1080/00268976.2017.1422811}} - -@phdthesis{Reb-THESIS-14, - Author = {E. Rebolini}, - School = {Universit\'e Pierre et Marie Curie}, - Title = {Range-separated density-functional theory for molecular excitation energies}, - Type = {{Th\`ese de doctorat}}, - Url = {https://tel.archives-ouvertes.fr/tel-01027522}, - Year = {2014}, - Bdsk-Url-1 = {https://tel.archives-ouvertes.fr/tel-01027522}} - -@phdthesis{Reb-THESIS-14_eng, - Author = {E. Rebolini}, - School = {Universit\'e Pierre et Marie Curie}, - Title = {Range-separated density-functional theory for molecular excitation energies}, - Type = {{PhD thesis}}, - Url = {https://tel.archives-ouvertes.fr/tel-01027522}, - Year = {2014}, - Bdsk-Url-1 = {https://tel.archives-ouvertes.fr/tel-01027522}} - -@article{RebTou-JCP-16, - Author = {E. Rebolini and J. Toulouse}, - Doi = {http://dx.doi.org/10.1063/1.4943003}, - Journal = {J. Chem. Phys.}, - Pages = {094107}, - Title = {Range-separated time-dependent density-functional theory with a frequency-dependent second-order Bethe-Salpeter correlation kernel}, - Volume = {144}, - Year = {2016}, - Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.4943003}} - -@misc{RebTou-JJJ-XX-note1, - Note = {The last two terms of the kernel in Eq. (31) of Ref.~\onlinecite{ZhaSteYan-JCP-13} contain non-antisymmetrized two-electron integrals. However, these terms can also be written with a factor of $1/2$ and antisymmetrized two-electron integrals, leading to our Eq.~(\ref{eq:eff kernel iajb}).}} - -@incollection{RebTouSav-INC-13, - Author = {E. Rebolini and J. Toulouse and A. Savin}, - Booktitle = {Electronic Structure and Reactivity}, - Editor = {S. K. Ghosh and P. K. Chattaraj}, - Note = {preprint at http://arxiv.org/abs/1304.1314}, - Pages = {367-390}, - Publisher = {CRC Press}, - Series = {Concepts and Methods in Modern Theoretical Chemistry Vol. 1}, - Title = {Electronic excitation energies of molecular systems from the Bethe-Salpeter equation: Example of the H$_2$ molecule}, - Year = {2013}} - -@misc{RebTouSav-JJJ-XX-note, - Note = {With the notations used here, the Hubbard model is obtained for $\Delta\varepsilon = 2 t$ and $J_{11}=J_{22}=J_{12}=J_{12}=K_{12}=U/2$ where $t$ is the hopping parameter and $U$ is the on-site Coulomb interaction.}} - -@article{RebTouTeaHelSav-JCP-14, - Author = {E. Rebolini and J. Toulouse and A. M. Teale and T. Helgaker and A. Savin}, - Doi = {http://dx.doi.org/10.1063/1.4890652}, - Journal = {Journal of Chemical Physics}, - Pages = {044123}, - Title = {Excitation energies along a range-separated adiabatic connection}, - Volume = {141}, - Year = {2014}, - Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.4890652}} - -@misc{RebTouTeaHelSav-JJJ-XX-sup, - Note = {See supplementary material at http://xxxxxxxx for the fits of the total and excitation energies.}} - -@article{RebTouTeaHelSav-MP-15, - Author = {E. Rebolini and J. Toulouse and A. M. Teale and T. Helgaker and A. Savin}, - Doi = {http://dx.doi.org/10.1080/00268976.2015.1011248}, - Journal = {Mol. Phys.}, - Pages = {1740}, - Title = {Excited states from range-separated density-functional perturbation theory}, - Volume = {113}, - Year = {2015}, - Bdsk-Url-1 = {http://dx.doi.org/10.1080/00268976.2015.1011248}} - -@article{RebTouTeaHelSav-PRA-15, - Author = {E. Rebolini and J. Toulouse and A. M. Teale and T. Helgaker and A. Savin}, - Doi = {http://dx.doi.org/10.1103/PhysRevA.91.032519}, - Journal = {Phys. Rev. A}, - Pages = {032519}, - Title = {Calculating excitation energies by extrapolation along adiabatic connections}, - Volume = {91}, - Year = {2015}, - Bdsk-Url-1 = {http://dx.doi.org/10.1103/PhysRevA.91.032519}} - -@article{RefJaiShaNeaKro-PRB-15, - Author = {Sivan Refaely-Abramson and Manish Jain and Sahar Sharifzadeh and Jeffrey B. Neaton and Leeor Kronik}, - Journal = {Phys. Rev. B}, - Pages = {081204(R)}, - Volume = {92}, - Year = {2015}} - -@article{RefShaGovAutNeaBaeKro-PRL-12, - Author = {S. Refaely-Abramson and Sahar Sharifzadeh and Niranjan Govind and Jochen Autschbach and Jeffrey B. Neaton and Roi Baer and Leeor Kronik}, - Journal = {Phys. Rev. Lett.}, - Pages = {226405}, - Volume = {109}, - Year = {2012}} - -@article{RegTha-JPB-84, - Author = {P. E. Regier and A. J. Thakkar}, - Journal = {J. Phys. B}, - Pages = {3391}, - Volume = {17}, - Year = {1984}} - -@article{ReiMal-JCP-98, - Author = {P. Reinhardt and J. P. Malrieu}, - Journal = {J. Chem. Phys.}, - Pages = {7632}, - Volume = {109}, - Year = {1998}} - -@article{ReiMal-JCP-99, - Author = {P. Reinhardt and J. P. Malrieu}, - Journal = {J. Chem. Phys.}, - Pages = {775}, - Volume = {110}, - Year = {1999}} - -@article{ReiMalPovRub-IJQC-97, - Author = {P. Reinhardt and J.-P. Malrieu and A. Povill and J. Rubio}, - Journal = {Int. J. Quantum Chem.}, - Pages = {167}, - Volume = {70}, - Year = {1997}} - -@article{ReiTho-ZP-25, - Author = {F. Reiche and W. Thomas}, - Journal = {Z. Phys.}, - Pages = {510}, - Volume = {34}, - Year = {1925}} - -@misc{ReiTouAngSav-JJJ-XX, - Author = {P. Reinhardt and J. Toulouse and J. G. \'Angy\'an and A. Savin}, - Note = {unpublished}} - -@incollection{ReiTouAssUmrHog-INC-12, - Address = {Washington, DC}, - Author = {P. Reinhardt and J. Toulouse and R. Assaraf and C. J. Umrigar and P. E. Hoggan}, - Booktitle = {Advances in Quantum Monte Carlo}, - Editor = {{S. Tanaka, S. M. Rothstein, and W. A. Lester, Jr.}}, - Pages = {53-63}, - Publisher = {American Chemical Society}, - Series = {ACS Symposium Series Vol. 1094}, - Title = {Quantum Monte Carlo Facing the Hartree-Fock Symmetry Dilemma: The Case of Hydrogen Rings}, - Year = {2012}} - -@article{ReiTouSav-TCA-18, - Author = {Peter Reinhardt and Julien Toulouse and Andreas Savin}, - Doi = {10.1007/s00214-018-2370-5}, - Journal = {Theor. Chem. Acc.}, - Pages = {168}, - Title = {Range-separated density-functional theory applied to the beryllium dimer and trimer}, - Volume = {137}, - Year = {2018}, - Bdsk-Url-1 = {https://doi.org/10.1007/s00214-018-2370-5}} - -@article{RenRinBluWieTkaSanReuSch-NJP-12, - Author = {Xinguo Ren and Patrick Rinke and Volker Blum and Jurgen Wieferink and Alexandre Tkatchenko and Andrea Sanfilippo and Karsten Reuter and Matthias Scheffler}, - Journal = {New J. Phys.}, - Pages = {053020}, - Volume = {14}, - Year = {2012}} - -@article{RenRinJoaSch-JMS-12, - Affiliation = {Fritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, 14195 Berlin, Germany}, - Author = {Ren, Xinguo and Rinke, Patrick and Joas, Christian and Scheffler, Matthias}, - Journal = {J. Mater. Sci.}, - Keyword = {Chemistry and Materials Science}, - Optnote = {10.1007/s10853-012-6570-4}, - Opturl = {http://dx.doi.org/10.1007/s10853-012-6570-4}, - Owner = {gambort}, - Pages = {7447}, - Publisher = {Springer Netherlands}, - Timestamp = {2012.07.06}, - Title = {Random-phase approximation and its applications in computational chemistry and materials science}, - Volume = {47}, - Year = {2012}} - -@article{RenRinSch-PRB-09, - Author = {Ren, Xinguo and Rinke, Patrick and Scheffler, Matthias}, - Doi = {10.1103/PhysRevB.80.045402}, - Journal = {Phys. Rev. B}, - Month = {Jul}, - Number = {4}, - Numpages = {8}, - Pages = {045402}, - Publisher = {American Physical Society}, - Title = {Exploring the random phase approximation: Application to CO adsorbed on Cu(111)}, - Volume = {80}, - Year = {2009}, - Bdsk-Url-1 = {https://doi.org/10.1103/PhysRevB.80.045402}} - -@article{RenTkaRinSch-PRL-11, - Author = {X. Ren and A. Tkatchenko and P. Rinke and M. Scheffler}, - Journal = {Phys. Rev. Lett.}, - Pages = {153003}, - Volume = {106}, - Year = {2011}} - -@article{ReyCepAldLes-JCP-82, - Author = {P. J. Reynolds and D. M. Ceperley and B. J. Alder and W. A. Lester}, - Journal = {J. Chem. Phys.}, - Pages = {5593}, - Title = {{Fixed-node quantum Monte Carlo for molecules}}, - Volume = {77}, - Year = {1982}} - -@article{ReyDupLes-JCP-85, - Author = {P. J. Reynolds and M. Dupuis and W. A. Lester}, - Journal = {J. Chem. Phys.}, - Pages = {1983}, - Volume = {82}, - Year = {1985}} - -@article{ReyOweLes-JCP-87, - Author = {P. J. Reynolds and R. K. Owen and W. A. Lester}, - Journal = {J. Chem. Phys.}, - Pages = {1905}, - Title = {{Is there a zeroth order time‐step error in diffusion quantum Monte Carlo?}}, - Volume = {{87}}, - Year = {1987}} - -@article{ReySav-IJQC-98, - Author = {J. Rey and A. Savin}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {581}, - Volume = {{69}}, - Year = {1998}} - -@article{RezDubJurHob-PCCP-15, - Author = {J. \v{R}ez\'a\v{c} and M. Dubeck\'y and P. Jure\v{c}ka and P. Hobza}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {19268}, - Volume = {17}, - Year = {2015}} - -@article{RezHob-JCTC-13, - Author = {J. \v{R}ez\'a\v{c} and P. Hobza}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2151}, - Volume = {9}, - Year = {2013}} - -@article{RezRilHob-JCTC-11, - Author = {J. \v{R}ez\'a\v{c} and K. E. Riley and P. Hobza}, - Journal = {J. Chem. Theory Comput.}, - Pages = {2427}, - Volume = {7}, - Year = {2011}} - -@article{RheHea-JPCA-07, - Author = {Y. M. Rhee and M. Head-Gordon}, - Journal = {J. Phys. Chem. A}, - Pages = {5314}, - Volume = {111}, - Year = {2007}} - -@article{RicAsh-PRB-94, - Author = {C. F. Richardson and N. W. Ashcroft}, - Journal = {Phys. Rev. B}, - Pages = {8170}, - Volume = {{50}}, - Year = {1994}} - -@article{RilAnd-MP-03, - Author = {K. E. Riley and J. B. Anderson}, - Journal = {Mol. Phys.}, - Pages = {3129}, - Volume = {101}, - Year = {2003}} - -@article{RocLuGal-JCP-10, - Author = {D. Rocca and D. Lu and G. Galli}, - Journal = {J. Chem. Phys.}, - Pages = {164109}, - Volume = {133}, - Year = {2010}} - -@article{RoeVes-IJQC-05, - Author = {I. R{\o}eggen and L. Veseth}, - Journal = {Int. J. Quantum Chem.}, - Pages = {201}, - Volume = {101}, - Year = {2005}} - -@article{RohGriBae-CPL-06, - Author = {D. Rohr and O. Gritsenko and E. J. Baerends}, - Journal = {Chem. Phys. Lett.}, - Pages = {336}, - Volume = {432}, - Year = {2006}} - -@article{RohHer-JCP-08, - Author = {M. A. Rohrdanz and J. M. Herbert}, - Journal = {J. Chem. Phys.}, - Pages = {034107}, - Volume = {129}, - Year = {2008}} - -@article{Roh-IJQC-00, - Author = {M. Rohlfing}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {807}, - Volume = {80}, - Year = {2000}} - -@article{RohLou-PRB-00, - Author = {M. Rohlfing and S. G. Louie}, - Journal = {Phys. Rev. B}, - Pages = {4927}, - Volume = {62}, - Year = {2000}} - -@article{RohLou-PRL-98, - Author = {M. Rohlfing and S. G. Louie}, - Journal = {Phys. Rev. Lett.}, - Pages = {3320}, - Volume = {80}, - Year = {1998}} - -@article{RohMarHer-JCP-09, - Author = {M. A. Rohrdanz and K. M. Martins and J. M. Herbert}, - Journal = {J. Chem. Phys.}, - Pages = {054112}, - Volume = {130}, - Year = {2009}} - -@article{RohPer-JCP-11, - Author = {D. R. Rohr and K. Pernal}, - Journal = {J. Chem. Phys.}, - Pages = {074104}, - Volume = {135}, - Year = {2011}} - -@article{RohTouPer-PRA-10, - Author = {D. R. Rohr and J. Toulouse and K. Pernal}, - Journal = {Phys. Rev. A}, - Pages = {052502}, - Title = {Combining density-functional theory and density-matrix-functional theory}, - Volume = {82}, - Year = {2010}} - -@article{RomGuyRei-JCP-09, - Author = {P. Romaniello and S. Guyot and L. Reining}, - Journal = {J. Chem. Phys.}, - Pages = {154111}, - Volume = {131}, - Year = {2009}} - -@article{RomSanBerSotMol-JCP-09, - Author = {P. Romaniello and D. Sangalli and J. A. Berger and F. Sottile and L. G. Molinari and L. Reining and G. Onida}, - Journal = {J. Chem. Phys.}, - Pages = {044108}, - Volume = {130}, - Year = {2009}} - -@article{RomSanBerSotMolReiOni-JCP-09, - Author = {P. Romaniello and D. Sangalli and J. A. Berger and F. Sottile and L. G. Molinari and L. Reining and G. Onida}, - Journal = {J. Chem. Phys.}, - Pages = {044108}, - Volume = {130}, - Year = {2009}} - -@article{RooTaySie-CP-80, - Author = {B. O. Roos and P. R. Taylor and P. E. M. Siegbahn}, - Journal = {Chem. Phys.}, - Pages = {157}, - Volume = {48}, - Year = {1980}} - -@article{RooSzuJas-TCA-87, - Author = {B. O. Roos and M. Szulkin and M. Jaszunski}, - Journal = {Theoret. Chim. Acta}, - Pages = {375}, - Volume = {71}, - Year = {1987}} - -@article{RosPauFulSto-PRB-99, - Author = {Krzysztof Ro\'sciszewski and Beate Paulus and Peter Fulde and Hermann Stoll}, - Journal = {Phys. Rev. B}, - Pages = {7905}, - Volume = {60}, - Year = {1999}} - -@article{Rot-CJC-13, - Author = {S. M. Rothstein}, - Journal = {Can. J. Chem.}, - Pages = {505}, - Title = {{A survey on pure sampling in quantum Monte Carlo methods}}, - Volume = {91}, - Year = {2013}} - -@article{RotVrb-JCP-87, - Author = {S. M. Rothstein and J. Vrbik}, - Journal = {J. Chem. Phys.}, - Pages = {1902}, - Title = {{A Green's function used in diffusion Monte Carlo}}, - Volume = {{87}}, - Year = {1987}} - -@article{Row-RMP-68, - Author = {D. J. Rowe}, - Journal = {Rev. Mod. Phys.}, - Pages = {153}, - Volume = {40}, - Year = {1968}} - -@article{RudSalHelAgr-JCP-05, - Author = {E. Rudberg and P. Sa{\l}ek and T. Helgaker and H. {\AA}agren}, - Journal = {J. Chem. Phys.}, - Pages = {184108}, - Volume = {123}, - Year = {2005}} - -@article{Rumer-32, - Author = {G. Rumer}, - Journal = {Nachr. Ges. Wiss. Goettingen, Math.-Phys. Kl.}, - Pages = {337}, - Year = {1932}} - -@article{RunGro-PRL-84, - Author = {E. Runge and E. K. U. Gross}, - Journal = {Phys. Rev. Lett.}, - Pages = {997}, - Volume = {52}, - Year = {1984}} - -@article{RuzPerCso-JCP-11, - Author = {A. Ruzsinsky and J. P. Perdew and G. I. Csonka}, - Journal = {J. Chem. Phys.}, - Pages = {114110}, - Volume = {134}, - Year = {2011}} - -@article{RuzPerCso-JCTC-10, - Author = {A. Ruzsinszky and J. P. Perdew and G. I. Csonka}, - Journal = {J. Chem. Theory Comput.}, - Pages = {127}, - Volume = {6}, - Year = {2010}} - -@article{RuzPerCsoVydScu-JCP-06, - Author = {A. Ruzsinszky and J. P. Perdew and G. I. Csonka and O. A. Vydrov and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {194112}, - Volume = {125}, - Year = {2006}} - -@article{RuzPerCsoVydScu-JCP-07, - Author = {A. Ruzsinszky and J. P. Perdew and G. I. Csonka and O. A. Vydrov and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {104102}, - Volume = {126}, - Year = {2007}} - -@article{SadBohCavEsrFabMacRau-JPB-00, - Author = {H R Sadeghpour and J L Bohn and M J Cavagnero and B D Esryk and I I Fabrikant and J H Macek and A R P Rau}, - Journal = {J. Phys. B,}, - Pages = {R93}, - Volume = {33}, - Year = {2000}} - -@article{SagPer-PRA-08, - Author = {E. Sagvolden and J. P. Perdew}, - Journal = {Phys. Rev. A}, - Pages = {012517}, - Volume = {77}, - Year = {2008}} - -@article{SahEhaNak-JCP-06, - Author = {B. Saha and M. Ehara and H. Nakatsuji}, - Journal = {J. Chem. Phys.}, - Pages = {014316}, - Volume = {125}, - Year = {2006}} - -@article{SaiTiaCheReb-PRB-08, - Author = {N. Sai and M. L. Tiago and J. R. Chelikowsky and F. A. Reboredo}, - Journal = {Phys. Rev. B}, - Pages = {161306}, - Volume = {77}, - Year = {2008}} - -@article{salvador:5046, - Author = {P. Salvador and I. Mayer}, - Issue = {11}, - Journal = {The Journal of Chemical Physics}, - Keywords = {SCF calculations; molecular electronic states; integration; density functional theory}, - Page = {5046-5052}, - Publisher = {AIP}, - Title = {Energy partitioning for ``fuzzy'' atoms}, - Url = {http://link.aip.org/link/?JCP/120/5046/1}, - Volume = {120}, - Year = {2004}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/120/5046/1}} - -@article{SamHar-JPB-06, - Author = {P. Samal and M. K. Harbola}, - Journal = {J. Phys. B}, - Pages = {4065}, - Volume = {39}, - Year = {2006}} - -@article{SanAda-PCCP-13, - Author = {J. C. Sancho-Garc\'ia and C. Adamo}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {14581}, - Volume = {15}, - Year = {2013}} - -@article{SanAraOrtOli-JCP-13, - Author = {J. C. Sancho-Garc\'ia and J. Arag\'o and E. Ort\'i and Y. Olivier}, - Journal = {J. Chem. Phys.}, - Pages = {204304}, - Volume = {138}, - Year = {2013}} - -@article{SanCivUsvTouShaMas-JCP-15, - Author = {G. Sansone and B. Civalleri and D. Usvyat and J. Toulouse and K. Sharkas and L. Maschio}, - Doi = {http://dx.doi.org/10.1063/1.4922996}, - Journal = {J. Chem. Phys.}, - Pages = {102811}, - Title = {Range-separated double-hybrid density-functional theory applied to periodic systems}, - Volume = {143}, - Year = {2015}, - Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.4922996}} - -@article{SanPer-JCP-09, - Author = {J. C. Sancho-Garc\'ia and A. J. P\'erez-Jim\'enez}, - Journal = {J. Chem. Phys.}, - Pages = {084108}, - Volume = {131}, - Year = {2009}} - -@article{SanPerMos-CPL-00, - Author = {J. C. Sancho-Garc\'ia and A. J. P\'erez-Jim\'enez and F. Moscard\'o}, - Journal = {Chem. Phys. Lett.}, - Pages = {245}, - Volume = {{317}}, - Year = {2000}} - -@article{SanPerSavBreAda-JPCA-16, - Author = {J. C. Sancho-Garc\'ia and A. J. P\'erez-Jim\'enez and M. Savarese and E. Br\'emond and C. Adamo}, - Journal = {J. Phys. Chem. A}, - Pages = {1756}, - Volume = {120}, - Year = {2016}} - -@article{San-PL-65, - Author = {E. A. Sanderson}, - Journal = {Phys. Lett.}, - Pages = {141}, - Volume = {19}, - Year = {1965}} - -@article{SanRomOniMar-JCP-11, - Author = {D. Sangalli and P. Romaniello and G. Onida and A. Marini}, - Journal = {J. Chem. Phys.}, - Pages = {034115}, - Title = {{Double excitations in correlated systems: A many-body approach}}, - Volume = {134}, - Year = {2011}} - -@article{SarDomAguUga-JCP-92, - Author = {C. Sarasola and L. Dominguez and M. Aguado and J. M. Ugalde}, - Journal = {J. Chem. Phys.}, - Pages = {6778}, - Volume = {96}, - Year = {1992}} - -@article{SarGalBue-CPC-99, - Author = {A. Sarsa and F. J. G\'alvez and E. Buend\'ia}, - Journal = {Comp. Phys. Comm.}, - Pages = {493}, - Volume = {121}, - Year = {1999}} - -@article{SarGalBue-JCP-98, - Author = {A. Sarsa and F. J. G\'alvez and E. Buend\'ia}, - Journal = {J. Chem. Phys.}, - Pages = {7075}, - Volume = {109}, - Year = {1998}} - -@article{SarUgaBoy-JPB-90, - Author = {C. Sarasola and J. M. Ugalde and R. J. Boyd}, - Journal = {J. Phys. B}, - Pages = {1095}, - Volume = {23}, - Year = {1990}} - -@article{SatNak-JCP-09, - Author = {T. Sato and H. Nakai}, - Journal = {J. Chem. Phys.}, - Pages = {224104}, - Volume = {131}, - Year = {2009}} - -@article{SatNak-JCP-10, - Author = {T. Sato and H. Nakai}, - Journal = {J. Chem. Phys.}, - Pages = {194101}, - Title = {{Local response dispersion method. II. Generalized multicenter interactions}}, - Volume = {133}, - Year = {2010}} - -@article{SauHel-JCC-02, - Author = {T. Saue and T. Helgaker}, - Journal = {J. Comput. Chem.}, - Pages = {814}, - Volume = {23}, - Year = {2002}} - -@incollection{Sau-INC-02, - Author = {Trond Saue}, - Booktitle = {Relativistic Electronic Structure Theory}, - Doi = {10.1016/S1380-7323(02)80033-4}, - Editor = {Peter Schwerdtfeger}, - Pages = {332-400}, - Publisher = {Elsevier}, - Title = {Post Dirac-Hartree-Fock methods -- properties}, - Year = {2002}, - Bdsk-Url-1 = {https://doi.org/10.1016/S1380-7323(02)80033-4}} - -@incollection{SauVis-INC-03, - Address = {Dordrecht}, - Author = {T. Saue and L. Visscher}, - Booktitle = {Theoretical Chemistry and Physics ofHeavy and Superheavy Elements}, - Editor = {S. Wilson and U. Kaldor}, - Pages = {211-267}, - Publisher = {Kluwer}, - Title = {Four-component electronic structure methods for molecules}, - Year = {2003}} - -@article{SavColAll-JCP-01, - Author = {A. Savin and F. Colonna and M. Allavena}, - Journal = {J. Chem. Phys.}, - Pages = {6827}, - Volume = {115}, - Year = {2001}} - -@article{SavCol-JMS-00a, - Author = {A. Savin and F. Colonna}, - Journal = {J. Mol. Struct. (Theochem)}, - Pages = {501}, - Volume = {{39}}, - Year = {2000}} - -@article{SavColPol-IJQC-03, - Author = {A. Savin and F. Colonna and R. Pollet}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {166}, - Title = {Adiabatic Connection Approach to Density Functional Theory of Electronic Systems}, - Volume = {{93}}, - Year = {2003}} - -@incollection{SavColTeu-INC-98, - Address = {New York}, - Author = {A. Savin and F. Colonna and J.-M. Teuler}, - Booktitle = {Electronic Density Functional Theory: Recent Progress and New Directions}, - Editor = {J. F. Dobson and G. Vignale and M. P. Das}, - Pages = {69}, - Publisher = {Plenum Press}, - Title = {Adiabatic Coupling in the Helium and the Beryllium Series}, - Year = {1998}} - -@article{Sav-CP-09, - Author = {A. Savin}, - Journal = {Chem. Phys.}, - Pages = {91}, - Volume = {356}, - Year = {2009}} - -@article{SavFla-IJQC-95, - Author = {A. Savin and H.-J. Flad}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {327}, - Volume = {{56}}, - Year = {1995}} - -@article{Sav-IJQC-88, - Author = {A. Savin}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {59}, - Volume = {{22}}, - Year = {1988}} - -@incollection{Sav-INC-91, - Address = {New York}, - Author = {A. Savin}, - Booktitle = {Density functional methods in chemistry}, - Editor = {J.K. Labanowski and J.W. Andzelm}, - Pages = {213}, - Publisher = {Springer-Verlag}, - Title = {Correlation contributions from density functionals}, - Year = {1991}} - -@incollection{Sav-INC-96a, - Author = {A. Savin}, - Booktitle = {Recent Advances in Density Functional Theory}, - Editor = {D. P. Chong}, - Pages = {129-148}, - Publisher = {World Scientific}, - Title = {Beyond the Kohn-Sham Determinant}, - Year = {1996}} - -@incollection{Sav-INC-96, - Address = {Amsterdam}, - Author = {A. Savin}, - Booktitle = {Recent Developments of Modern Density Functional Theory}, - Editor = {J. M. Seminario}, - Pages = {327-357}, - Publisher = {Elsevier}, - Title = {On Degeneracy, Near Degeneracy and Density Functional Theory}, - Year = {1996}} - -@article{Sav-JCP-11, - Author = {A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {214108}, - Volume = {134}, - Year = {2011}} - -@article{Sav-JCP-14, - Author = {A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {18A509}, - Volume = {140}, - Year = {2014}} - -@article{Sav-JCP-89, - Author = {A. Savin}, - Journal = {J. chim. phys.}, - Pages = {757}, - Volume = {{86}}, - Year = {1989}} - -@article{Sav-JCTC-09, - Author = {A. Savin}, - Journal = {J. Chem. Theory Comput.}, - Pages = {822}, - Volume = {5}, - Year = {2009}} - -@incollection{SavStoPre-INC-84, - Address = {New York}, - Author = {A. Savin}, - Booktitle = {Local Density Approximations in Quantum Chemistry and Solid State Physics}, - Editor = {J. P. Dahl and J. Avery}, - Pages = {263}, - Publisher = {Plenum}, - Year = {1984}} - -@article{SavStoPre-TCA-86, - Author = {A. Savin and H. Stoll and H. Preuss}, - Journal = {Theor. Chim. Acta}, - Pages = {407}, - Volume = {{70}}, - Year = {1986}} - -@misc{Sce-ARX-09, - Author = {A. Scemama}, - Note = {\url{http://arxiv.org/abs/0909.5012v1}}} - -@article{SceBenJacCafLoo-JCP-18, - Author = {A. Scemama and A. Benali and D. Jacquemin and M. Caffarel and P.-F. Loos}, - Journal = {J. Chem. Phys.}, - Pages = {034108}, - Title = {Excitation energies from diffusion Monte Carlo using selected configuration interaction nodes}, - Volume = {149}, - Year = {2018}} - -@misc{SceFil-ARX-XX, - Author = {A. Scemama and C. Filippi}, - Url = {http://arxiv.org/abs/cond-mat/0511278}, - Bdsk-Url-1 = {http://arxiv.org/abs/cond-mat/0511278}} - -@article{SceFil-PRB-06, - Author = {A. Scemama and C. Filippi}, - Journal = {Phys. Rev. B}, - Pages = {241101}, - Volume = {73}, - Year = {2006}} - -@article{Sch-AP-59, - Author = {C. Schwartz}, - Journal = {Ann. Phys. (N.Y.)}, - Pages = {156}, - Volume = {6}, - Year = {1959}} - -@article{SchBalBoaElbGorJenKosMatNguSuWinDupMon-JCC-93, - Author = {M. W. Schmidt and K. K. Baldridge and J. A. Boatz and S. T. Elbert and M. S. Gordon and J. H. Jensen and S. Koseki and N. Matsunaga and K. A. Nguyen and S. J. Su and T. L. Windus and M. Dupuis and J. A. Montgomery}, - Journal = {J. Comput. Chem.}, - Pages = {1347}, - Volume = {{14}}, - Year = {1993}} - -@article{SchBudFil-JCP-04, - Author = {Friedemann Schautz and F. Buda and Claudia Filippi}, - Journal = {J. Chem. Phys.}, - Pages = {5836}, - Volume = {121}, - Year = {2004}} - -@article{SchDidElsSunGurChaLiWin-JCIM-07, - Author = {K. L. Schuchardt and B. T. Didier and T. Elsethagen and L. Sun and V. Gurumoorthi and J. Chase and J. Li and T. L. Windus}, - Journal = {J. Chem. Inf. Model.}, - Pages = {1045}, - Volume = {47}, - Year = {2007}} - -@article{SchFah-JCP-02, - Author = {Friedemann Schautz and Stephen Fahy}, - Journal = {J. Chem. Phys.}, - Pages = {3533}, - Volume = {116}, - Year = {2002}} - -@article{SchFil-JCP-04, - Author = {F. Schautz and C. Filippi}, - Journal = {J. Chem. Phys.}, - Pages = {10931}, - Title = {{Optimized Jastrow-Slater wave functions for ground and excited states: Application to the lowest states of ethene}}, - Volume = {120}, - Year = {2004}} - -@article{SchGor-ARPC-98, - Author = {M. W. Schmidt and M. S. Gordon}, - Journal = {Annu. Rev. Phys. Chem.}, - Pages = {233}, - Title = {{The construction and interpretation of MCSCF wavefunctions}}, - Volume = {49}, - Year = {1998}} - -@article{SchGriBae-JCP-99, - Author = {P.R.T. Schipper and O.V. Gritsenko and E.J. Baerends}, - Journal = {J. Chem. Phys.}, - Pages = {4056}, - Volume = {{111}}, - Year = {1999}} - -@article{SchGriBae-TCA-98, - Author = {P. R. T. Schipper and O. V. Gritsenko and E. J. Baerends}, - Journal = {Theor. Chem. Acc.}, - Pages = {329}, - Volume = {99}, - Year = {1998}} - -@article{SchGriGisBae-JCP-00, - Author = {{P. R. T. Schipper, O. V. Gritsenko, S. J. A. van Gisbergen, and E. J. Baerends}}, - Journal = {J. Chem. Phys.}, - Pages = {1344}, - Volume = {112}, - Year = {2000}} - -@article{SchGri-PCCP-06, - Author = {T. Schwabe and S. Grimme}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {4398}, - Title = {Towards chemical accuracy for thermodynamics of large molecules:new hybrid density functionals including non-local correlation effects}, - Volume = {8}, - Year = {2006}} - -@article{SchGri-PCCP-07, - Author = {T. Schwabe and S. Grimme}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {3397}, - Volume = {9}, - Year = {2007}} - -@article{SchHetWer-JCP-99, - Author = {M. Sch\"utz and G. Hetzer and H.-J. Werner}, - Journal = {J. Chem. Phys.}, - Pages = {5691}, - Volume = {111}, - Year = {1999}} - -@incollection{Sch-INC-63, - Address = {New York and London}, - Author = {C. Schwartz}, - Booktitle = {Methods in Computational Physics, Vol. 2}, - Editor = {B. Alder and S. Fernbach and M. Rotenberg}, - Pages = {241-266}, - Publisher = {Academic Press}, - Year = {1963}} - -@incollection{Sch-INC-87, - Address = {Berlin Heidelberg}, - Author = {K. E. Schmidt}, - Booktitle = {Models and Methods in Few-Body Physics, Lecture Notes in Physics Vol. 273}, - Editor = {L. S. Ferreira and A. C. Fonseca and L. Streit}, - Pages = {363-407}, - Publisher = {Springer}, - Title = {{Variational and Green's function Monte Carlo calculations of few-body systems}}, - Year = {1987}} - -@article{SchKoc-PRA-00, - Author = {R. Schnabel and M. Kock}, - Journal = {Phys. Rev. A}, - Pages = {062506}, - Volume = {61}, - Year = {2000}} - -@article{Sch-PR-62, - Author = {C. Schwartz}, - Journal = {Phys. Rev.}, - Pages = {1015}, - Volume = {126}, - Year = {1962}} - -@article{Sch-PRA-82, - Author = {J. Schirmer}, - Journal = {Phys. Rev. A}, - Pages = {2395}, - Volume = {26}, - Year = {1982}} - -@article{Sch-PRB-97, - Author = {Arno Schindlmayr}, - Journal = {Phys. Rev. B}, - Pages = {3528}, - Volume = {{56}}, - Year = {1997}} - -@article{Sch-SCI-86, - Author = {H. F. Schaefer}, - Journal = {Science}, - Pages = {1100}, - Volume = {231}, - Year = {1986}} - -@article{SchZhaTru-JPCA-05, - Author = {N. E. Schultz and Y. Zhao and D. G. Truhlar}, - Journal = {J. Phys. Chem. A}, - Pages = {11127}, - Volume = {109}, - Year = {2005}} - -@article{ScuAya-JCP-99, - Author = {G. E. Scuseria and P. Y. Ayala}, - Journal = {J. Chem. Phys.}, - Pages = {8330}, - Title = {{Linear scaling coupled cluster and perturbation theories in the atomic orbital basis}}, - Volume = {111}, - Year = {1999}} - -@article{ScuHenSor-JCP-08, - Author = {G. E. Scuseria and T. M. Henderson and D. C. Sorensen}, - Journal = {J. Chem. Phys.}, - Pages = {231101}, - Volume = {129}, - Year = {2008}} - -@article{SeiGorSav-PRA-07, - Author = {M. Seidl and P. Gori-Giorgi and A. Savin}, - Journal = {Phys. Rev. A}, - Pages = {042511}, - Volume = {75}, - Year = {2007}} - -@article{SeiGorVogMajLev-PRB-96, - Author = {A. Seidl and A. G\"orling and P. Vogl and J. A. Majewski and M. Levy}, - Journal = {Phys. Rev. B}, - Pages = {3764}, - Volume = {53}, - Year = {1996}} - -@article{SeiPerKur-PRA-00, - Author = {M. Seidl and John P. Perdew and S. Kurth}, - Journal = {Phys. Rev. A}, - Pages = {012502}, - Volume = {62}, - Year = {2000}} - -@article{SeiPerKur-PRL-00, - Author = {M. Siedl and J. P. Perdew and S. Kurth}, - Journal = {Phys. Rev. Lett.}, - Pages = {5070}, - Volume = {84}, - Year = {2000}} - -@article{SeiPerLev-PRA-99, - Author = {M. Seidl and J. P. Perdew and M. Levy}, - Journal = {Phys. Rev. A}, - Pages = {51}, - Volume = {59}, - Year = {1999}} - -@article{SekMaeKamHir-JCP-07, - Author = {H. Sekino and Y. Maeda and M. Kamiya and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {014107}, - Volume = {126}, - Year = {2007}} - -@article{SekMaeKam-MP-05, - Author = {H. Sekino and Y. Maeda and M. Kamiya}, - Journal = {Mol. Phys.}, - Pages = {2183}, - Volume = {103}, - Year = {2005}} - -@article{SenHedAlaKneFro-MP-16, - Author = {B. Senjean and E. D. Hedeg{\aa}rd and Md. M. Alam and S. Knecht and E. Fromager}, - Journal = {Mol. Phys.}, - Pages = {968}, - Volume = {114}, - Year = {2016}} - -@article{SenKneJenFro-PRA-15, - Author = {B. Senjean and S. Knecht and H. J. Aa. Jensen and E. Fromager}, - Journal = {Phys. Rev. A}, - Pages = {012518}, - Volume = {92}, - Year = {2015}} - -@article{ShaDewLatGro-PRB-08, - Author = {S. Sharma and J. K. Dewhurst and N. N. Lathiotakis and E. K. U. Gross}, - Journal = {Phys. Rev. B}, - Pages = {201103(R)}, - Title = {Reduced density matrix functional for many-electron systems}, - Volume = {78}, - Year = {2008}} - -@article{ShaHib-Angew09, - Author = {W. Wu and J. Gu and J. Song and S. Shaik and P. C. Hiberty}, - Journal = {Angew. Chem. Int. Ed.}, - Pages = {1407}, - Volume = {48}, - Year = {2009}} - -@book{ShaHib-BOOK-08, - Author = {S. Shaik and P. C. Hiberty}, - Publisher = {John Wiley \& Sons, Inc}, - Title = {A Chemist's Guide to Valence Bond Theory}, - Year = {2008}} - -@article{ShaHib-ChemEurJ07, - Author = {S. Shaik and D. Danovich and B. Silvi and D. L. Lauvergnat and P. C. Hiberty}, - Journal = {Chem. Eur. J.}, - Pages = {6358}, - Volume = {11}, - Year = {2005}} - -@article{ShaHib-NatChem09, - Author = {S. Shaik and D. Danovich and W. Wu and P. C. Hiberty}, - Journal = {Nat. Chem.}, - Pages = {443}, - Volume = {1}, - Year = {2009}} - -@article{ShaHor-PR-53, - Author = {R. T. Sharp and G. K. Horton}, - Journal = {Phys. Rev.}, - Pages = {317}, - Volume = {90}, - Year = {1953}} - -@incollection{Sha-INC-71, - Address = {New York}, - Author = {L. J. Sham}, - Booktitle = {Computational Methods in Band Theory}, - Editor = {P. Marcus and J. F. Janak and A. R. Williams}, - Publisher = {Plenum}, - Year = {1971}} - -@article{Sha-PRA-70, - Author = {L. J. Sham}, - Journal = {Phys. Rev. A}, - Pages = {969}, - Volume = {1}, - Year = {1970}} - -@article{ShaSavJenTou-JCP-12, - Author = {K. Sharkas and A. Savin and H. J. Aa. Jensen and J. Toulouse}, - Journal = {J. Chem. Phys.}, - Pages = {044104}, - Title = {A multiconfigurational hybrid density-functional theory}, - Volume = {137}, - Year = {2012}} - -@article{ShaSch-PRL-83, - Author = {L. J. Sham and M. Schl\"uter}, - Journal = {Phys. Rev. Lett.}, - Pages = {1888}, - Volume = {51}, - Year = {1983}} - -@article{ShaShu-Angew-99, - Author = {S. Shaik and A. Shurki}, - Journal = {Angew. Chem. Int. Ed.}, - Pages = {586}, - Volume = {38}, - Year = {1999}} - -@article{ShaTha-JPB-84, - Author = {B. S. Sharma and A. J. Thakkar}, - Journal = {J. Phys. B}, - Pages = {3405}, - Volume = {17}, - Year = {1984}} - -@article{ShaTouMasCiv-JCP-14, - Author = {K. Sharkas and J. Toulouse and L. Maschio and B. Civalleri}, - Journal = {J. Chem. Phys.}, - Pages = {044105}, - Title = {Double-hybrid density-functional theory applied to molecular crystals}, - Volume = {141}, - Year = {2014}} - -@article{ShaTouSav-JCP-11, - Author = {K. Sharkas and J. Toulouse and A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {064113}, - Title = {Double-hybrid density-functional theory made rigorous}, - Volume = {134}, - Year = {2011}} - -@article{SheBooGruAla-PRB-12, - Author = {Shepherd, James J. and Booth, George and Grueneis, Andreas and Alavi, Ali}, - Journal = {{Phys. Rev. B}}, - Number = {{8}}, - Title = {{Full configuration interaction perspective on the homogeneous electron gas}}, - Volume = {{85}}, - Year = {{2012}}} - -@article{SheHenScu-PRL-14, - Author = {James J. Shepherd and Thomas M. Henderson and Gustavo E. Scuseria}, - Journal = {Phys. Rev. Lett.}, - Pages = {133002}, - Volume = {112}, - Year = {2014}} - -@article{SheKneSau-PCCP-15, - Author = {A. Shee and S. Knecht and T. Saue}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {10978}, - Volume = {17}, - Year = {2015}} - -@article{SheLeiVanSch-JCP-98, - Author = {C. D. Sherrill and M. L. Leininger and T. J. Van Huis and H. F. Schaefer}, - Journal = {J. Chem. Phys.}, - Pages = {1040}, - Volume = {108}, - Year = {1998}} - -@article{SheMenGriBae-JCP-13, - Author = {X. W. Sheng and {\L}. M. Mentel and O. V. Gritsenko and E. J. Baerends}, - Journal = {J. Chem. Phys.}, - Pages = {164105}, - Volume = {138}, - Year = {2013}} - -@article{SheShaSim-JCP-82, - Author = {R. Shepard and I. Shavitt and J. Simons}, - Journal = {J. Chem. Phys.}, - Pages = {543}, - Volume = {76}, - Year = {1982}} - -@article{ShiHirHir-PRA-06, - Author = {Yasuteru Shigeta and Kimihiko Hirao and So Hirata}, - Journal = {Phys. Rev. A}, - Pages = {010502}, - Volume = {73}, - Year = {2006}} - -@article{ShiMar-PRB-93, - Author = {E. L. Shirley and R. M. Martin}, - Journal = {Phys. Rev. B}, - Pages = {15404}, - Volume = {47}, - Year = {1993}} - -@article{ShiMck-JCP-71, - Author = {T.-I. Shibuya and V. McKoy}, - Journal = {J. Chem. Phys.}, - Pages = {1738}, - Volume = {54}, - Year = {1971}} - -@article{ShiMck-PRA-70, - Author = {T.-I. Shibuya and V. McKoy}, - Journal = {Phys. Rev. A}, - Pages = {2208}, - Volume = {2}, - Year = {1979}} - -@misc{Shi-UNP-XX, - Note = {We used the code of E. Shirley to generate norm-conserving Hartree-Fock pseudopotential according to the construction of D. Vanderbilt, Phys. Rev. B {\bf 32}, 8412 (1985).}} - -@article{Sini-90, - Author = {G. Sini and G. Ohanessian and P. C. Hiberty and S. S. Shaik}, - Journal = {J. Am. Chem. Soc.}, - Pages = {1407}, - Volume = {112}, - Year = {1990}} - -@article{Sin-JCP-62, - Author = {O. Sinano\u{g}lu}, - Journal = {J. Chem. Phys.}, - Pages = {3198}, - Volume = {{36}}, - Year = {1962}} - -@article{SinShe-JPCA-04, - Author = {M. O. Sinnokrot and C. D. Sherrill}, - Journal = {J. Phys. Chem. A}, - Pages = {10200}, - Volume = {108}, - Year = {2004}} - -@article{SinTosLanSjo-PR-68, - Author = {K. S. Singwi and M. P. Tosi and R. H. Land and A. Sj\"{o}lander}, - Journal = {Phys. Rev.}, - Pages = {589}, - Volume = {{176}}, - Year = {1968}} - -@article{SinValShe-JACS-02, - Author = {M. O. Sinnokrot and E. F. Valeev and C. D. Sherrill}, - Journal = {J. Am. Chem. Soc.}, - Pages = {10887}, - Volume = {124}, - Year = {2002}} - -@article{SisAbaMauGaaSchLop-JCP-16, - Author = {Adonay Sissay and Paul Abanador and F. Mauger and Mette Gaarde and Kenneth J. Schafer and Kenneth Lopata}, - Journal = {J. Chem. Phys.}, - Pages = {094105}, - Volume = {145}, - Year = {2016}} - -@article{SlaManWilWoo-PR-69, - Author = {J. Slater and J.B. Mann and T.M. Wilson and J.H. Wood}, - Journal = {Phys. Rev.}, - Pages = {672}, - Volume = {184}, - Year = {1969}} - -@article{Sla-PR-51, - Author = {J. C. Slater}, - Journal = {Phys. Rev.}, - Pages = {385}, - Volume = {81}, - Year = {1951}} - -@article{SliKry-JCP-02, - Author = {L. V. Slipchenko and A. I. Krylov}, - Journal = {J. Chem. Phys.}, - Pages = {4694}, - Volume = {117}, - Year = {2002}} - -@article{SmiDelBukGraFab-JCC-16, - Author = {{S. \'Smiga, F. Della Sala, A. Buksztel, I. Grabowski, E. Fabiano}}, - Journal = {J. Comput. Chem.}, - Pages = {2081}, - Title = {Accurate Kohn--Sham ionization potentials from scaled-opposite-spin second-order optimized effective potential methods}, - Volume = {37}, - Year = {2016}} - -@article{SmiFraMusBukGraLupTou-JCP-16, - Author = {S. \'Smiga and O. Franck and B. Mussard and A. Buksztel and I. Grabowski and E. Luppi and J. Toulouse}, - Doi = {http://dx.doi.org/10.1063/1.4964319}, - Journal = {J. Chem. Phys.}, - Pages = {144102}, - Title = {Self-consistent double-hybrid density-functional theory using the optimized-effective-potential method}, - Volume = {145}, - Year = {2016}, - Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.4964319}} - -@article{SnaRot-JCP-00, - Author = {M. Snajdr and S. M. Rothstein}, - Journal = {J. Chem. Phys.}, - Pages = {4935}, - Volume = {112}, - Year = {2000}} - -@misc{SnyRupHanMulBur-ARX-11, - Author = {John C. Snyder and Matthias Rupp and Katja Hansen and Klaus-Robert M\"uller and Kieron Burke}, - Note = {\url{http://arxiv.org/abs/1112.5441}}} - -@article{SodKecYagHir-JCP-13, - Author = {Olaseni Sode and Murat Ke\c{c}eli and Kiyoshi Yagi and So Hirata}, - Journal = {J. Chem. Phys.}, - Pages = {074501}, - Volume = {138}, - Year = {2013}} - -@article{SongMoWu-JCC-08, - Author = {L. Song and J. Song and Y. Mo and W. Wu}, - Journal = {J. Comput. Chem.}, - Pages = {399}, - Volume = {30}, - Year = {2008}} - -@article{SonMoZhaWu-JCC-05, - Author = {L. Song and Y. Mo and Q. Zhang and W. Wu}, - Journal = {J. Comput. Chem.}, - Pages = {514}, - Volume = {26}, - Year = {2005}} - -@article{SonTokSatWatHir-JCP-07, - Author = {J.-W. Song and S. Tokura and T. Sato and M. A. Watson and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {154109}, - Volume = {127}, - Year = {2007}} - -@article{SonWatHir-JCP-09, - Author = {J.-W. Song and M. A. Watson and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {144108}, - Volume = {131}, - Year = {2009}} - -@article{SonWatNakHir-JCP-08, - Author = {J.-W. Song and M. A. Watson and A. Nakata and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {184113}, - Volume = {129}, - Year = {2008}} - -@article{SonWatSekHir-JCP-08, - Author = {J.-W. Song and M. A. Watson and H. Sekino and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {024117}, - Volume = {129}, - Year = {2008}} - -@article{SonWuZhaSha-JCC-04, - Author = {L. Song and W. Wu and Q. Zhang and S. Shaik}, - Journal = {J. Comput. Chem.}, - Pages = {472}, - Volume = {25}, - Year = {2004}} - -@article{SonYamHir-JCP-11, - Author = {J.-W. Song and K. Yamashita and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {135}, - Volume = {2011}, - Year = {071103}} - -@article{SorCap-JCP-10, - Author = {S. Sorella and L. Capriotti}, - Journal = {J. Chem. Phys.}, - Pages = {234111}, - Volume = {133}, - Year = {2010}} - -@article{SorCasRoc-JCP-07, - Author = {S. Sorella and M. Casula and D. Rocca}, - Journal = {J. Chem. Phys.}, - Pages = {014105}, - Volume = {127}, - Year = {2007}} - -@article{Sor-PRB-01, - Author = {S. Sorella}, - Journal = {Phys. Rev. B}, - Pages = {024512}, - Volume = {64}, - Year = {2001}} - -@article{Sor-PRB-05, - Author = {S. Sorella}, - Journal = {Phys. Rev. B}, - Pages = {241103}, - Title = {{Wave function optimization in the variational Monte Carlo method}}, - Volume = {71}, - Year = {2005}} - -@article{SotOleRei-PRL-03, - Author = {F. Sottile and V. Olevano and L. Reining}, - Journal = {Phys. Rev. Lett.}, - Pages = {056402}, - Volume = {91}, - Year = {2003}} - -@article{SouShaTou-JCP-14, - Author = {Sidi M. O. Souvi and Kamal Sharkas and Julien Toulouse}, - Journal = {J. Chem. Phys.}, - Pages = {084107}, - Title = {Double-hybrid density-functional theory with meta-generalized-gradient approximations}, - Volume = {140}, - Year = {2014}} - -@misc{SouShaTou-JJJ-XX-sup, - Note = {See supplementary material.}} - -@article{SpiMalMayZur-TCA-XX, - Author = {F. Spiegelmann and J. P. Malrieu and D. Maynau and J. P. Zurru}, - Journal = {Theoret. Chim. Acta}} - -@article{StaDav-CPL-01, - Author = {Viktor N. Staroverov and Ernest R. Davidson}, - Journal = {Chem. Phys. Lett.}, - Pages = {142}, - Title = {A density functional method for degenerate spin-multiplet components}, - Volume = {340}, - Year = {2001}} - -@article{StaScuPerDavKat-PRA-06, - Author = {V. N. Staroverov and G. E. Scuseria and J. P. Perdew and E. R. Davidson and J. Katriel}, - Journal = {Phys. Rev. A}, - Pages = {044501}, - Volume = {74}, - Year = {2006}} - -@article{StaScuPerTaoDav-PRA-04, - Author = {Viktor N. Staroverov and Gustavo E. Scuseria and John P. Perdew and Jianmin Tao and Ernest R. Davidson}, - Journal = {Phys. Rev. A}, - Pages = {012502}, - Volume = {70}, - Year = {2004}} - -@article{StaScuTaoPer-JCP-03, - Author = {V. N. Staroverov and G. E. Scuseria and J. Tao and J. P. Perdew}, - Journal = {J. Chem. Phys.}, - Pages = {12129}, - Volume = {119}, - Year = {2003}} - -@article{SteAltFroDec-CP-97, - Author = {{M. Stener, G. De Alti, G. Fronzoni, P. Decleva}}, - Journal = {Chem. Phys.}, - Pages = {197}, - Volume = {222}, - Year = {1997}} - -@article{SteAutGovKroBae-JPCL-12, - Author = {T. Stein and J. Autschbach and N. Govind and L. Kronik and R. Baer}, - Journal = {J. Phys. Chem. Lett.}, - Pages = {3740}, - Volume = {3}, - Year = {2012}} - -@article{SteCor-JCTC-11, - Author = {S. N. Steinmann and C. Corminboeuf}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3567}, - Title = {Comprehensive Benchmarking of a Density-Dependent Dispersion Correction}, - Volume = {7}, - Year = {2011}} - -@article{SteDecGor-JCP-01, - Author = {M. Stener and P. Decleva and A. G\"orling}, - Journal = {J. Chem. Phys.}, - Pages = {7816}, - Volume = {114}, - Year = {2001}} - -@article{SteDec-JCP-00, - Author = {M. Stener and P. Decleva}, - Journal = {J. Chem. Phys.}, - Pages = {10871}, - Volume = {112}, - Year = {2000}} - -@article{SteDec-JPB-97, - Author = {M. Stener and P. Decleva}, - Journal = {J. Phys. B,}, - Pages = {4481}, - Volume = {30}, - Year = {1997}} - -@article{SteDecLis-JPB-95, - Author = {M. Stener and P. Decleva and A. Lisini}, - Journal = {J. Phys. B,}, - Pages = {4973}, - Volume = {28}, - Year = {1995}} - -@article{SteDevChaFri-JPC-94, - Author = {P. J. Stephens and F. J. Devlin and C. F. Chabalowski and M. J. Frisch}, - Journal = {J. Phys. Chem.}, - Pages = {11623}, - Title = {Ab Initio Calculation of Vibrational Absorption and Circular Dichroism Spectra Using Density Functional Force Fields}, - Volume = {98}, - Year = {1994}} - -@article{SteFroDec-JCP-05, - Author = {M. Stener and G. Fronzoni and P. Decleva}, - Journal = {J. Chem. Phys.}, - Pages = {234301}, - Volume = {122}, - Year = {2005}} - -@article{Ste-JCP-70, - Author = {R. F. Stewart}, - Journal = {J. Chem. Phys.}, - Pages = {431}, - Volume = {52}, - Year = {1970}} - -@article{SteKroBae-JACS-09, - Author = {T. Stein and L. Kronik and R. Baer}, - Journal = {J. Am. Chem. Soc.}, - Pages = {2818}, - Volume = {131}, - Year = {2009}} - -@article{SteKroBae-JCP-09, - Author = {T. Stein and L. Kronik and R. Baer}, - Journal = {J. Chem. Phys.}, - Pages = {244119}, - Volume = {131}, - Year = {2009}} - -@book{SteLee-BOOK-13, - Author = {{G. Stefanucci and R. van Leeuwen}}, - Publisher = {Cambridge University Press}, - Title = {Nonequilibrium Many-Body Theory of Quantum Systems: A Modern Introduction}, - Year = {2013}} - -@article{SteTofFroDec-JCP-06, - Author = {M. Stener and D. Toffoli and G. Fronzoni and P. Decleva}, - Journal = {J. Chem. Phys.}, - Pages = {114306}, - Volume = {124}, - Year = {2006}} - -@article{SteTofFroDec-TCA-07, - Author = {M. Stener and D. Toffoli and G. Fronzoni and P. Decleva}, - Journal = {Theor. Chem. Acc.}, - Pages = {943}, - Volume = {117}, - Year = {2007}} - -@article{SteYan-JCP-13, - Author = {S. N. Steinmann and W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {074107}, - Volume = {139}, - Year = {2013}} - -@article{Sto-CPL-03, - Author = {H. Stoll}, - Journal = {Chem. Phys. Lett.}, - Pages = {141}, - Title = {On the coupling of multi-configuration self-consistent-field and density-functional information}, - Volume = {{376}}, - Year = {2003}} - -@article{StoGolPre-TCA-80, - Author = {H. Stoll and C.M.E. Pavlidou and H. Preuss}, - Journal = {Theor. Chim. Acta}, - Pages = {29}, - Volume = {{55}}, - Year = {1980}} - -@article{StoPavPre-TCA-78, - Author = {H. Stoll and C.M.E. Pavlidou and H. Preuss}, - Journal = {Theor. Chim. Acta}, - Pages = {143}, - Volume = {{49}}, - Year = {1978}} - -@incollection{StoSav-INC-85, - Address = {New York}, - Author = {H. Stoll and A. Savin}, - Booktitle = {Density Functional Methods in Physics}, - Editor = {R. M. Dreizler and J. da Providencia}, - Pages = {177-207}, - Publisher = {Plenum}, - Title = {Density Functionals for Correlation Energies of Atoms and Molecules}, - Year = {1985}} - -@article{StoTeaTouHelFro-JCP-13, - Author = {Alexandrina Stoyanova and Andrew M. Teale and Julien Toulouse and Trygve Helgaker and Emmanuel Fromager}, - Journal = {J. Chem. Phys.}, - Pages = {134113}, - Title = {Alternative separation of exchange and correlation energies in multi-configuration range-separated density-functional theory}, - Volume = {139}, - Year = {2013}} - -@article{StrKumCorSagTeaHel-JCP-11, - Author = {Marie D. Str{\o}msheim and N. Kumar and S. Coriani and E. Sagvolden and Andrew M. Teale and Trygve Helgaker}, - Journal = {J. Chem. Phys.}, - Pages = {194109}, - Volume = {135}, - Year = {2011}} - -@article{Str-RNC-88, - Author = {G. Strinati}, - Journal = {Rivista del Nuovo Cimento}, - Pages = {1}, - Volume = {11}, - Year = {1988}} - -@article{SucDra-PRA-79, - Author = {J. Sucher and R. J. Drachman}, - Journal = {Phys. Rev. A}, - Pages = {424}, - Volume = {21}, - Year = {1979}} - -@article{Suc-PRA-80, - Author = {J. Sucher}, - Journal = {Phys. Rev. A}, - Pages = {348}, - Volume = {22}, - Year = {1980}} - -@article{SuePurZhaKraWal-PRB-07, - Author = {M. Suewattana and W. Purwanto and S. Zhang and H. Krakauer and E. J. Walter}, - Journal = {Phys. Rev. B}, - Pages = {245123}, - Volume = {75}, - Year = {2007}} - -@article{Suh-CPL-83, - Author = {S. Suhai}, - Journal = {Chem. Phys. Lett.}, - Pages = {619}, - Volume = {96}, - Year = {1983}} - -@article{SuLiTru-JCP-16, - Author = {Haoyu S. Yu and Shaohong L. Li and Donald G. Truhlar}, - Journal = {J. Chem. Phys.}, - Pages = {130901}, - Volume = {145}, - Year = {2016}} - -@article{SulNorSau-MP-12, - Author = {D. Sulzer and P. Norman and T. Saue}, - Journal = {Mol. Phys.}, - Pages = {2535}, - Volume = {110}, - Year = {2012}} - -@article{SunMarCsoRuzHaoKimKrePer-PRB-11, - Author = {Jianwei Sun and Martijn Marsman and Gabor I. Csonka and Adrienn Ruzsinszky and Pan Hao and Yoon-Suk Kim and Georg Kresseand John P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {035117}, - Volume = {84}, - Year = {2011}} - -@article{SunRuzPer-PRL-15, - Author = {Jianwei Sun and Adrienn Ruzsinszky and John P. Perdew}, - Journal = {Phys. Rev. Lett.}, - Pages = {036402}, - Title = {Strongly Constrained and Appropriately Normed Semilocal Density Functional}, - Volume = {115}, - Year = {2015}} - -@article{SuSongWuHibSha-JCC-07, - Author = {P. Su and L. Song and W. Wu and P. C. Hiberty and S. Shaik}, - Journal = {J. Comput. Chem.}, - Pages = {185}, - Volume = {28}, - Year = {2007}} - -@article{SuXu-JCTC-15, - Author = {N. Q. Su and X. Xu}, - Journal = {J. Chem. Theory Comput.}, - Pages = {4677}, - Volume = {11}, - Year = {2015}} - -@article{SuXu-MP-16, - Author = {N. Q. Su and X. Xu}, - Journal = {Mol. Phys.}, - Pages = {1207}, - Volume = {114}, - Year = {2016}} - -@article{SuYanMorXu-JPCA-14, - Author = {N. Q. Su and W. Yang and P. Mori-S\'anchez and X. Xu}, - Journal = {J. Phys. Chem. A}, - Pages = {9201}, - Volume = {118}, - Year = {2014}} - -@article{SveBar-IJQC-95, - Author = {P. S. Svendsen and U. von Barth}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {351}, - Volume = {{56}}, - Year = {1995}} - -@article{SzaMul-CR-12, - Author = {P. G. Szalay and T. M\"uller and G. Gidofalvi and H. Lischka and R. Shepard}, - Journal = {Chem. Rev.}, - Pages = {112}, - Title = {Multiconfiguration Self-Consistent Field and Multireference Configuration Interaction Methods and Applications}, - Volume = {108}, - Year = {2012}} - -@book{SzaOst-BOOK-96, - Address = {New York}, - Author = {A. Szabo and N. S. Ostlund}, - Publisher = {Dover}, - Title = {Modern Quantum Chemistry: Introduction to Advanced Electronic Structure Theory}, - Year = {1996}} - -@article{SzaOst-IJQC-77, - Author = {A. Szabo and N. S. Ostlund}, - Journal = {Int. J. Quantum Chem.}, - Pages = {389}, - Volume = {S11}, - Year = {1977}} - -@article{SzaOst-JCP-77, - Author = {A. Szabo and N. S. Ostlund}, - Journal = {J. Chem. Phys.}, - Pages = {4351}, - Volume = {67}, - Year = {1977}} - -@article{SzaPfeMurBarVerSchLeg-IJQC-15, - Author = {S. Szalay and M. Pfeffer and V. Murg and G. Barcza and F. Verstraete and R. Schneider and O. Legeza}, - Journal = {Int. J. Quantum Chem.}, - Pages = {1342}, - Title = {Tensor Product Methods and Entanglement Optimization for Ab Initio Quantum Chemistry}, - Volume = {{115}}, - Year = {2015}} - -@article{TacMorSuzIgu-IJQC-98, - Author = {M. Tachikawa and K. Mori and K. Suzuki and K. Iguchi}, - Journal = {Int. J. Quantum Chem.}, - Pages = {491}, - Volume = {70}, - Year = {1998}} - -@article{TacOsa-JCP-00, - Author = {M. Tachikawa and Y. Osamura}, - Journal = {J. Chem. Phys.}, - Pages = {4942}, - Volume = {113}, - Year = {2000}} - -@article{TacTanMor-IJQC-99, - Author = {M. Tachikawa and K. Taneda and K. Mori}, - Journal = {Int. J. Quantum Chem.}, - Pages = {497}, - Volume = {75}, - Year = {1999}} - -@article{TakHohMalMarShe-JCP-10, - Author = {T. Takatani and E. G. Hohenstein and M. Malagoli and M. S. Marshall and C. D. Sherrill}, - Journal = {J. Chem. Phys.}, - Pages = {144104}, - Volume = {132}, - Year = {2010}} - -@article{TakYamYam-CPL-02, - Author = {R. Takeda and S. Yamanaka and K. Yamaguchi}, - Journal = {Chem. Phys. Lett.}, - Pages = {321}, - Volume = {366}, - Year = {2002}} - -@article{TakYamYam-IJQC-03, - Author = {R. Takeda and S. Yamanaka and K. Yamaguchi}, - Journal = {Int. J. Quantum Chem.}, - Pages = {317}, - Title = {Fractional Occupation Numbers and Spin Density Functional Calculations of Degenerate Systems}, - Volume = {{93}}, - Year = {2003}} - -@article{TakYamYam-IJQC-04, - Author = {R. Takeda and S. Yamanaka and K. Yamaguchi}, - Journal = {Int. J. Quantum Chem.}, - Pages = {463}, - Volume = {{96}}, - Year = {2004}} - -@article{TakYas-PRB-91, - Author = {Y. Takada and H. Yasuhara}, - Journal = {Phys. Rev. B}, - Pages = {7879}, - Volume = {{44}}, - Year = {1991}} - -@article{Tal-PRL-86, - Author = {James D. Talman}, - Journal = {Phys. Rev. Lett.}, - Pages = {1091}, - Volume = {57}, - Year = {1989}} - -@article{TalSha-PRA-76, - Author = {J. D. Talman and W. F. Shadwick}, - Journal = {Phys. Rev. A}, - Pages = {36}, - Volume = {14}, - Year = {1976}} - -@article{TanKobYamYosYam-JCP-89, - Author = {K. Tanaka and H. Kobayashi and S. Yamanaka and K. Yoshizawa and T. Yamaba}, - Journal = {J. Chem. Phys.}, - Pages = {3724}, - Volume = {91}, - Year = {1989}} - -@article{TanToe-JCP-03, - Author = {K. T. Tang and J. P. Toennies}, - Journal = {J. Chem. Phys.}, - Pages = {4976}, - Volume = {118}, - Year = {2003}} - -@article{TaoPerStaScu-PRL-03, - Author = {J. Tao and J. P. Perdew and V. N. Staroverov and G. E. Scuseria}, - Journal = {Phys. Rev. Lett.}, - Pages = {146401}, - Volume = {91}, - Year = {2003}} - -@article{TapTavRotFilCas-JCP-08, - Author = {E. Tapavicza and I. Tavernelli and U. Rothlisberger and C. Filippi and M. E. Casida}, - Journal = {J. Chem. Phys.}, - Pages = {124108}, - Volume = {129}, - Year = {2008}} - -@article{TarKarSerVuzMar-JPCA-08, - Author = {Alex Tarnopolsky and Amir Karton and Rotem Sertchook and Dana Vuzman and Jan M. L. Martin}, - Journal = {J. Phys. Chem. A}, - Pages = {3}, - Volume = {112}, - Year = {2008}} - -@article{TawTsuYanYanHir-JCP-04, - Author = {Y. Tawada and T. Tsuneda and S. Yanagisawa and T. Yanai and K. Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {8425}, - Title = {A long-range-corrected time-dependent density functional theory}, - Volume = {{120}}, - Year = {2004}} - -@article{TayAngGalZhaGygHirSonRahLilPodBulHenScuTouPevTruSza-JCP-16, - Author = {Taylor, D. E. and \'Angy\'an, J. G. and Galli, G. and Zhang, C. and Gygi, F. and Hirao, K. and Song, J. W. and Rahul, K. and von Lilienfeld, O. A. and Podeszwa, R. and Bulik, I. W. and Henderson, T. M. and Scuseria, G. E. and Toulouse, J. and Peverati, R. and Truhlar, D. G. and Szalewicz, K.}, - Journal = {J. Chem. Phys.}, - Pages = {124105}, - Title = {Blind test of density-functional-based methods on intermolecular interaction energies}, - Volume = {145}, - Year = {2016}} - -@book{TDDFT-BOOK-06, - Address = {Berlin}, - Editor = {M. L. Marques and C. A. Ullrich and F. Nogueira and A. Rubio and K. Burke and E. K. U. Gross}, - Publisher = {Springer}, - Series = {Lecture Notes in Physics Vol. 706}, - Title = {Time-Dependent Density Functional Theory}, - Year = {2006}} - -@book{TDDFT-BOOK-12, - Address = {Berlin}, - Editor = {M. A. L. Marques and N. T. Maitra, F. M. S. Nogueira, E. K. U. Gross, A. Rubio}, - Publisher = {Springer}, - Series = {Lecture Notes in Physics Vol. 837}, - Title = {Fundamentals of Time-Dependent Density Functional Theory}, - Year = {2012}} - -@article{TeaCorHel-JCP-09, - Author = {A. M. Teale and S. Coriani and T. Helgaker}, - Journal = {J. Chem. Phys.}, - Pages = {104111}, - Title = {{The calculation of adiabatic-connection curves from full configuration-interaction densities: Two-electron systems}}, - Volume = {130}, - Year = {2009}} - -@article{TeaCorHel-JCP-10b, - Author = {Andrew M. Teale and S. Coriani and Trygve Helgaker}, - Journal = {J. Chem. Phys.}, - Pages = {164112}, - Volume = {133}, - Year = {2010}} - -@article{TeaCorHel-JCP-10, - Author = {Andrew M. Teale and S. Coriani and Trygve Helgaker}, - Journal = {J. Chem. Phys.}, - Pages = {164115}, - Volume = {132}, - Year = {2010}} - -@article{TeaDepToz-JCP-08, - Author = {{A. M. Teale, F. De Proft, and D. J. Tozer}}, - Journal = {J. Chem. Phys.}, - Pages = {044110}, - Volume = {129}, - Year = {2008}} - -@article{TecGomEksVis-PCCP-11, - Author = {P. Tecmer and A. S. P. Gomes and U. Ekstr\"om and L. Visscher}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {6249}, - Volume = {13}, - Year = {2011}} - -@article{TelKvaSagEksTeaHel-PRA-12, - Author = {E. I. Tellgren and S. Kvaal and E. Sagvolden and U. Ekstr\"om and A. M. Teale and T. Helgaker}, - Journal = {Phys. Rev. A}, - Pages = {062506}, - Volume = {86}, - Year = {2012}} - -@article{TelSosRozChu-PRA-13, - Author = {D. A. Telnov and K. E. Sosnova and E. Rozenbaum and S.-I. Chu}, - Journal = {Phys. Rev. A}, - Pages = {053406}, - Volume = {87}, - Year = {2013}} - -@article{Tha-CPL-03, - Author = {A. J. Thakkar}, - Journal = {Chem. Phys. Lett.}, - Pages = {80}, - Volume = {381}, - Year = {2003}} - -@incollection{Tha-INC-87, - Address = {Dordrecht}, - Author = {A. J. Thakkar}, - Booktitle = {Density Matrices and Density Functionals}, - Editor = {R. M. Erdahl and V. H. Smith}, - Pages = {553-581}, - Publisher = {Reidel}, - Year = {1987}} - -@article{ThaSmi-CPL-76, - Author = {A. J. Thakkar and V. H. Smith}, - Journal = {Chem. Phys. Lett.}, - Pages = {476}, - Volume = {42}, - Year = {1976}} - -@article{ThaSmi-JCP-77, - Author = {A. J. Thakkar and V. H. Smith}, - Journal = {J. Chem. Phys.}, - Pages = {1191}, - Volume = {67}, - Year = {1977}} - -@article{ThaTriSmi-IJQC-84, - Author = {A. J. Thakkar and A. N. Tripathi and V. H. Smith}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {157}, - Volume = {26}, - Year = {1984}} - -@article{ThaTriSmi-PRA-84, - Author = {A. J. Thakkar and A. N. Tripathi and V. H. Smith}, - Journal = {Phys. Rev. A}, - Pages = {1108}, - Volume = {29}, - Year = {1984}} - -@book{Tho-BOOK-61, - Address = {New York}, - Author = {D. J. Thouless}, - Publisher = {Academic Press}, - Title = {The Quantum Mechanics of Many Body Systems}, - Year = {1961}} - -@article{Tho-NAT-25, - Author = {W. Thomas}, - Journal = {Naturwissenschaften}, - Pages = {627}, - Volume = {13}, - Year = {1925}} - -@article{Tho-NP-61, - Author = {D. J. Thouless}, - Journal = {Nucl. Phys.}, - Pages = {78}, - Volume = {22}, - Year = {1961}} - -@article{ThyFleJen-JCP-08, - Author = {J. Thyssen and T. Fleig and H. J. Aa. Jensen}, - Journal = {J. Chem. Phys.}, - Pages = {034109}, - Volume = {129}, - Year = {2008}} - -@article{TiaChe-PRB-06, - Author = {M. L. Tiago and J. R. Chelikowsky}, - Journal = {Phys. Rev. B}, - Pages = {205334}, - Volume = {73}, - Year = {2006}} - -@article{TiaChe-SSC-05, - Author = {M. L. Tiago and J. R. Chelikowsky}, - Journal = {Solid State Commun.}, - Pages = {333}, - Volume = {136}, - Year = {2005}} - -@article{TiaKenHooReb-JCP-08, - Author = {M. L. Tiago and P. R. C. Kent and R. Q. Hood and F. A. Reboredo}, - Journal = {J. Chem. Phys.}, - Pages = {084311}, - Volume = {129}, - Year = {2008}} - -@article{TkaSch-PRL-09, - Author = {A. Tkatchenko and M. Scheffler}, - Journal = {Phys. Rev. Lett.}, - Pages = {073005}, - Title = {{Accurate molecular van der Waals interactions from ground-state electron density and free-atom reference data}}, - Volume = {102}, - Year = {2009}} - -@article{TofSteDec-PRA-06, - Author = {D. Toffoli and M. Stener and P. Decleva}, - Journal = {Phys. Rev. A}, - Pages = {042704}, - Volume = {73}, - Year = {2006}} - -@article{ToiWoo-PRB-70, - Author = {F. Toigo and T. O. Woodruff}, - Journal = {Phys. Rev. B}, - Pages = {3958}, - Volume = {{2}}, - Year = {1970}} - -@article{ToiWoo-PRB-71, - Author = {F. Toigo and T. O. Woodruff}, - Journal = {Phys. Rev. B}, - Pages = {371}, - Volume = {{4}}, - Year = {1971}} - -@incollection{Tos-INC-99, - Address = {University of Oxford}, - Author = {M. P. Tosi}, - Booktitle = {Electron Correlation in the Solid State}, - Editor = {N. H. March}, - Publisher = {World Scientific Publishing Company}, - Title = {Many-Body Effects in Jellium}, - Year = {1999}} - -@incollection{TouAssUmr-INC-16, - Author = {J. Toulouse and R. Assaraf and C. J. Umrigar}, - Booktitle = {Electron Correlation in Molecules - ab initio Beyond Gaussian Quantum Chemistry}, - Doi = {10.1016/bs.aiq.2015.07.003}, - Editor = {P. E. Hoggan and T. Ozdogan}, - Pages = {285-314}, - Publisher = {Academic Press}, - Series = {Advances in Quantum Chemistry Vol. 73}, - Title = {Introduction to the Variational and Diffusion Monte Carlo Methods}, - Year = {2016}, - Bdsk-Url-1 = {https://doi.org/10.1016/bs.aiq.2015.07.003}} - -@article{TouAssUmr-JCP-07, - Author = {J. Toulouse and R. Assaraf and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {244112}, - Title = {{Zero-variance zero-bias quantum Monte Carlo estimators of the spherically and system-averaged pair density}}, - Volume = {126}, - Year = {2007}} - -@incollection{TouCafReiHogUmr-INC-12, - Address = {Dordrecht Heidelberg London New York}, - Author = {J. Toulouse and M. Caffarel and P. Reinhardt and P. E. Hoggan and C. J. Umrigar}, - Booktitle = {Advances in the Theory of Quantum Systems in Chemistry and Physics}, - Editor = {P. E. Hoggan and J. Maruani and P. Piecuch and G. Delgado-Barrio and E. J. Br\"andas}, - Pages = {345-353}, - Publisher = {Springer}, - Series = {Progress in Theoretical Chemistry and Physics Vol. 22}, - Title = {Quantum Monte Carlo calculations of electronic excitation energies: The case of the singlet $n\to\pi^*$ (CO) transition in acrolein}, - Year = {2012}} - -@article{TouColSav-JCP-05, - Author = {J. Toulouse and F. Colonna and A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {014110}, - Title = {Short-range exchange and correlation energy density functionals: Beyond the local-density approximation}, - Volume = {122}, - Year = {2005}} - -@misc{TouColSav-JJJ-XXa, - Author = {J. Toulouse and F. Colonna and A. Savin}, - Title = {in preparation}} - -@article{TouColSav-MP-05, - Author = {Julien Toulouse and Francois Colonna and Andreas Savin}, - Journal = {Mol. Phys.}, - Pages = {2725}, - Title = {Exchange-correlation potentials and local energies per particle along non-linear adiabatic connections}, - Volume = {103}, - Year = {2005}} - -@article{TouColSav-PRA-04, - Author = {J. Toulouse and F. Colonna and A. Savin}, - Journal = {Phys. Rev. A}, - Keywords = {density functional theory; wave functions; exchange interactions (electron); electron correlations}, - Number = {6}, - Pages = {062505}, - Publisher = {APS}, - Title = {Long-range--short-range separation of the electron-electron interaction in density-functional theory}, - Volume = {70}, - Year = {2004}} - -@misc{TouGerJanSavAng-JJJ-XX-note, - Note = {For Ne$_{2}$ at equilibrium distance with aug-cc-pVQZ basis, the counterpoise correction on the interaction energy is 16 $\mu$H for RSH+RPAx and 62 $\mu$H for standard MP2.}} - -@article{TouGerJanSavAng-PRL-09, - Author = {J. Toulouse and I. C. Gerber and G. Jansen and A. Savin and J. G. \'Angy\'an}, - Journal = {Phys. Rev. Lett.}, - Pages = {096404}, - Title = {Adiabatic-connection fluctuation-dissipation density-functional theory based on range separation}, - Volume = {102}, - Year = {2009}} - -@article{TouGorSav-IJQC-06, - Author = {J. Toulouse and P. Gori-Giorgi and A. Savin}, - Journal = {Int. J. Quantum Chem.}, - Pages = {2026}, - Title = {Scaling relations, virial theorem and energy densities for long-range and short-range density functionals}, - Volume = {106}, - Year = {2006}} - -@article{TouGorSav-TCA-05, - Author = {J. Toulouse and P. Gori-Giorgi and A. Savin}, - Journal = {Theor. Chem. Acc.}, - Pages = {305}, - Volume = {114}, - Year = {2005}} - -@misc{Tou-JJJ-XX, - Author = {S. Dubillard and E. Eliav and L. Visscher and R. Bast and T. Saue}, - Note = {unpublished}} - -@article{Tou-PRB-05, - Author = {Julien Toulouse}, - Journal = {Phys. Rev. B}, - Pages = {035117}, - Title = {Simple model of the static exchange-correlation kernel of a uniform electron gas with long-range electron-electron interaction}, - Volume = {72}, - Year = {2005}} - -@article{TouRebGouDobSeaAng-JCP-13, - Author = {Julien Toulouse and Elisa Rebolini and Tim Gould and John F. Dobson and Prasenjit Seal and J\'anos G. \'Angy\'an}, - Journal = {J. Chem. Phys.}, - Pages = {194106}, - Title = {Assessment of range-separated time-dependent density-functional theory for calculating $C_6$ dispersion coefficients}, - Volume = {138}, - Year = {2013}} - -@article{TouSavFla-IJQC-04, - Author = {J. Toulouse and A. Savin and H.-J. Flad}, - Journal = {Int. J. Quantum Chem.}, - Pages = {1047}, - Title = {Short-range exchange-correlation energy of a uniform electron gas with modified electron-electron interaction}, - Volume = {100}, - Year = {2004}} - -@misc{TouSav-JJJ-XX, - Author = {J. Toulouse and A. Savin}, - Title = {in preparation}} - -@article{TouSav-JMS-06, - Author = {Julien Toulouse and Andreas Savin}, - Journal = {J. Mol. Struct. (Theochem)}, - Pages = {147}, - Title = {Local density approximation for long-range or for short-range energy functionals?}, - Volume = {762}, - Year = {2006}} - -@article{TouShaBreAda-JCP-11, - Author = {J. Toulouse and K. Sharkas and E. Br\'emond and C. Adamo}, - Journal = {J. Chem. Phys.}, - Pages = {101102}, - Title = {Rationale for a new class of double-hybrid approximations in density-functional theory}, - Volume = {135}, - Year = {2011}} - -@phdthesis{Tou-THESIS-05, - Author = {J. Toulouse}, - Note = {tel.archives-ouvertes.fr/tel-00550772}, - School = {Universit\'e Pierre et Marie Curie (Paris 6)}, - Year = {2005}} - -@article{TouUmr-JCP-07, - Author = {J. Toulouse and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {084102}, - Title = {{Optimization of quantum Monte Carlo wave functions by energy minimization}}, - Volume = {126}, - Year = {2007}} - -@article{TouUmr-JCP-08, - Author = {J. Toulouse and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {174101}, - Title = {{Full optimization of Jastrow-Slater wave functions with application to the first-row atoms and homonuclear diatomic molecules}}, - Volume = {128}, - Year = {2008}} - -@misc{TouUmr-JJJ-XX, - Author = {J. Toulouse and C. J. Umrigar}, - Note = {unpublished}} - -@misc{TouZhuAngSav-JJJ-XX-note2, - Note = {In the context of density-functional theory RPA is usually derived from the Kohn-Sham reference, while in the context of many-body perturbation theory (see appendices) RPA is usually derived from the HF reference. Therefore, both PBE+RPA and HF+RPA are theoretically justified.}} - -@misc{TouZhuAngSav-JJJ-XX-note3, - Note = {The inverse of a 4-point function $\chi (1,2;1',2')$ is defined according to $\int d1'd2' \chi (1,2;1',2') \chi^{-1} (2',1';4,3) = \delta(1,3) \delta (2,4)$.}} - -@misc{TouZhuAngSav-JJJ-XX-note, - Note = {The short-range self-energy correction $\Delta \Sigma^\sr_\l$ is wrongly missing in Eq.~(11) of Ref.~\onlinecite{TouGerJanSavAng-PRL-09}. However, in practice, this term vanishes in the RPA or RPAx approximation so that the results of Ref.~\onlinecite{TouGerJanSavAng-PRL-09} are correct.}} - -@article{TouZhuAngSav-PRA-10, - Author = {Julien Toulouse and Wuming Zhu and J\'anos G. \'Angy\'an and Andreas Savin}, - Journal = {Phys. Rev. A}, - Pages = {032502}, - Title = {Range-separated density-functional theory with the random-phase approximation: Detailed formalism and illustrative applications}, - Volume = {82}, - Year = {2010}} - -@article{TouZhuSavJanAng-JCP-11, - Author = {J. Toulouse and W. Zhu and A. Savin and G. Jansen and J. G. \'Angy\'an}, - Journal = {J. Chem. Phys.}, - Pages = {084119}, - Title = {Closed-shell ring coupled cluster doubles theory with range separation applied on weak intermolecular interactions}, - Volume = {135}, - Year = {2011}} - -@misc{TouZhuSavJanAng-JJJ-XX, - Author = {J. Toulouse and W. Zhu and A. Savin and G. Jansen and J. G. \'Angyan}, - Note = {unpublished}} - -@misc{TouZhuSavJanAng-JJJ-XX-note, - Note = {In Ref.~\onlinecite{Hes-JCP-11}, AC-RPA, NRPA1, NRPA3, and NRPA4 refer to what we call here RPAx-I, RPAx-II, RPA-SO2, and RPA-SO1, respectively. In addition, NRPA2 corresponds to the variant of Fukuda {\it et al.}, i.e. $2E_{c,\RPAxII}-E_{c,\text{MP2}}$.}} - -@article{TowZupCau-CPC-96, - Author = {M. D. Towler and A. Zupan and M. Caus\'a}, - Journal = {Comp. Phys. Comm.}, - Pages = {181}, - Volume = {98}, - Year = {1996}} - -@article{TozHan-JCP-98, - Author = {D. J. Tozer and N. C. Handy}, - Journal = {J. Chem. Phys.}, - Pages = {10180}, - Volume = {109}, - Year = {1998}} - -@article{Tri-JPB-80, - Author = {H. P. Trivedi}, - Journal = {J. Phys. B}, - Pages = {839}, - Volume = {13}, - Year = {1980}} - -@article{Tru-CPL-98, - Author = {D. G. Truhlar}, - Journal = {Chem. Phys. Lett.}, - Pages = {45}, - Volume = {294}, - Year = {1998}} - -@article{TsuScu-JCP-11, - Author = {T. Tsuchimochi and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {064101}, - Volume = {134}, - Year = {2011}} - -@article{TsuScuSav-JCP-10, - Author = {T. Tsuchimochi and G. E. Scuseria and A. Savin}, - Journal = {J. Chem. Phys.}, - Pages = {024111}, - Volume = {132}, - Year = {2010}} - -@article{TsuSonSuzHir-JCP-10, - Author = {Takao Tsuneda and Jong-Won Song and Satoshi Suzuki and Kimihiko Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {174101}, - Volume = {133}, - Year = {2010}} - -@article{TsuSuzHir-JCP-99, - Author = {Takao Tsuneda and Toshihisa Suzumura and Kimihiko Hirao}, - Journal = {J. Chem. Phys.}, - Pages = {5656}, - Volume = {111}, - Year = {1999}} - -@article{UgaBoy-IJQC-85, - Author = {J. M. Ugalde and R. J. Boyd}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {439}, - Volume = {27}, - Year = {1985}} - -@book{Ull-BOOK-11, - Author = {Carsten A. Ullrich}, - Publisher = {OUP Oxford}, - Title = {Time-Dependent Density-Functional Theory: Concepts and Applications}, - Year = {2011}} - -@article{UllKoh-PRL-01, - Author = {C. A. Ullrich and W. Kohn}, - Journal = {Phys. Rev. Lett.}, - Pages = {093001}, - Volume = {87}, - Year = {2001}} - -@article{UmrFil-PRL-05, - Author = {C. J. Umrigar and C. Filippi}, - Journal = {Phys. Rev. Lett.}, - Pages = {150201}, - Title = {{Energy and variance optimization of many-body wave functions}}, - Volume = {94}, - Year = {2005}} - -@misc{UmrFil-PRL-05-note, - Note = {The convergence in 2 iterations, mentioned near the end of Ref.~\onlinecite{UmrFil-PRL-05} was obtained using the correlated sampling adjustment of $a_\diag$ and the TU Hessian.}} - -@incollection{UmrGon-INC-93, - Address = {Singapore}, - Author = {C. J. Umrigar and X. Gonze}, - Booktitle = {High Performance Computing and its Application to the Physical Sciences, Proceedings of the Mardi Gras '93 Conference}, - Editor = {D. A. Browne {\it et al.}}, - Publisher = {World Scientific}, - Year = {1993}} - -@article{UmrGon-PRA-94, - Author = {C. J. Umrigar and X. Gonze}, - Journal = {Phys. Rev. A}, - Pages = {3827}, - Volume = {50}, - Year = {1994}} - -@article{Umr-IJQC-89, - Author = {C. J. Umrigar}, - Journal = {Int. J. Quantum Chem.}, - Pages = {217}, - Volume = {{23}}, - Year = {1989}} - -@incollection{Umr-INC-99, - Address = {Dordrecht}, - Author = {C. J. Umrigar}, - Booktitle = {Quantum Monte Carlo Methods in Physics and Chemistry}, - Editor = {M. P. Nightingale and C. J. Umrigar}, - Pages = {129}, - Publisher = {Kluwer}, - Series = {NATO ASI Ser. C 525}, - Year = {1999}} - -@article{UmrNigRun-JCP-93, - Author = {C. J. Umrigar and M. P. Nightingale and K. J. Runge}, - Journal = {J. Chem. Phys.}, - Pages = {2865}, - Title = {{A diffusion Monte Carlo algorithm with very small time-step errors}}, - Volume = {99}, - Year = {1993}} - -@article{Umr-PRL-93, - Author = {C. J. Umrigar}, - Journal = {Phys. Rev. Lett.}, - Pages = {408}, - Title = {{Accelerated Metropolis method}}, - Volume = {71}, - Year = {1993}} - -@incollection{UmrSavGon-INC-98, - Author = {Umrigar, C.J. and Savin, A. and Gonze, Xavier}, - Booktitle = {Electronic Density Functional Theory}, - Doi = {10.1007/978-1-4899-0316-7_12}, - Editor = {Dobson, John F. and Vignale, Giovanni and Das, Mukunda P.}, - Pages = {167-176}, - Publisher = {Springer US}, - Title = {Are Unoccupied Kohn-Sham Eigenvalues Related to Excitation Energies?}, - Year = {1998}, - Bdsk-Url-1 = {https://doi.org/10.1007/978-1-4899-0316-7_12}} - -@article{UmrTouFilSorHen-PRL-07, - Author = {C. J. Umrigar and J. Toulouse and C. Filippi and S. Sorella and R. G. Hennig}, - Journal = {Phys. Rev. Lett.}, - Pages = {110201}, - Title = {Alleviation of the Fermion-sign problem by optimization of many-body wave functions}, - Volume = {98}, - Year = {2007}} - -@misc{Umr-UNP-XXb, - Author = {C. J. Umrigar}, - Note = {unpublished}} - -@misc{Umr-UNP-XX, - Author = {C. J. Umrigar}, - Note = {unpublished}} - -@misc{Umr-UNP-XX_fr, - Author = {C. J. Umrigar}, - Note = {non publi{\'e}}} - -@incollection{UmrWilWil-INC-88, - Address = {Berlin}, - Author = {C. J. Umrigar and K. G. Wilson and J. W. Wilkins}, - Booktitle = {Computer Simulation Studies in Condensed Matter Physics: Recent Developments}, - Editor = {D. P. Landau and K. K. Mon and H. B. Sch\"uttler}, - Publisher = {Springer}, - Year = {1988}} - -@article{UmrWilWil-PRL-88, - Author = {C. J. Umrigar and K. G. Wilson and J. W. Wilkins}, - Journal = {Phys. Rev. Lett.}, - Pages = {1719}, - Title = {{Optimized trial wave functions for quantum Monte Carlo calculations}}, - Volume = {60}, - Year = {1988}} - -@article{UtsIch-PRB-80a, - Author = {K. Utsumi and S. Ichimaru}, - Journal = {Phys. Rev. B}, - Pages = {1522}, - Volume = {{22}}, - Year = {1980}} - -@article{UtsIch-PRB-80, - Author = {K. Utsumi and S. Ichimaru}, - Journal = {Phys. Rev. B}, - Pages = {5203}, - Volume = {{22}}, - Year = {1980}} - -@article{Val-JCP-80a, - Author = {S. M. Valone}, - Journal = {J. Chem. Phys.}, - Pages = {4653}, - Volume = {73}, - Year = {1980}} - -@phdthesis{Van-THESIS-18, - Author = {Marco Vanzini}, - School = {{\'E}cole Polytechnique, Universit{\'e} Paris-Saclay}, - Title = {Auxiliary systems for observables: dynamical local connector approximation for electron addition and removal spectra}, - Year = {2018}} - -@article{VasSin-PRB-72, - Author = {P. Vashista and K.S. Singwi}, - Journal = {Phys. Rev. B}, - Pages = {875}, - Volume = {{6}}, - Year = {1972}} - -@article{VeiCle-JCP-69, - Author = {A. Veillard and E. Clementi}, - Journal = {J. Chem. Phys.}, - Pages = {2415}, - Volume = {{49}}, - Year = {1969}} - -@article{VitDelGor-JCP-05, - Author = {{V. Vitale, F. Della Sala, and A. G\"orling}}, - Journal = {J. Chem. Phys.}, - Pages = {244102}, - Volume = {122}, - Year = {2005}} - -@phdthesis{Vog-THESIS-03, - Author = {M. Vogt}, - School = {University of Cambridge}, - Title = {Spectral Moments in the Homogeneous Electron Gas}, - Year = {2003}} - -@article{VogZimNee-PRB-04, - Author = {M. Vogt and R. Zimmermann and R. J. Needs}, - Journal = {Phys. Rev. B}, - Pages = {045113}, - Volume = {{69}}, - Year = {2004}} - -@article{VosWilNus-CJP-80, - Author = {S. J. Vosko and L. Wilk and M. Nusair}, - Journal = {Can. J. Phys.}, - Pages = {1200}, - Volume = {{58}}, - Year = {1980}} - -@article{VrbDepRot-JCP-88, - Author = {J. Vrbik and M. F. DePasquale and S. M. Rothstein}, - Journal = {J. Chem. Phys.}, - Pages = {3784}, - Volume = {88}, - Year = {1988}} - -@article{VutCamGurHutparPatPetSpaDoyGabDem-JPB-10, - Author = {A. C. Vutha and W. C. Campbell and Y. V. Gurevich and N. R. Hutzler and M. Parsons and D. Patterson and E. Petrik and B. Spaun and J. M. Doyle and G. Gabrielse and D. DeMille}, - Journal = {J. Phys. B}, - Pages = {074007}, - Volume = {43}, - Year = {2010}} - -@article{VydScu-JCP-06, - Author = {O. A. Vydrov and G. E. Scuseria}, - Journal = {J. Chem. Phys.}, - Pages = {234109}, - Volume = {125}, - Year = {2006}} - -@article{VydScuPer-JCP-07, - Author = {Vydrov, O. A. and Scuseria, G. E. and Perdew, J. P.}, - Journal = {J. Chem. Phys.}, - Pages = {154109}, - Title = {Tests of functionals for systems with fractional electron number}, - Volume = {126}, - Year = {2007}} - -@article{VydVoo-JCP-09, - Author = {O. A. Vydrov and T. van Voorhis}, - Journal = {J. Chem. Phys.}, - Pages = {104105}, - Volume = {130}, - Year = {2009}} - -@article{VydVoo-JCP-10b, - Author = {O. A. Vydrov and T. V. Voorhis}, - Journal = {J. Chem. Phys.}, - Pages = {244103}, - Title = {{Nonlocal van der Waals density functional: The simpler the better}}, - Volume = {133}, - Year = {2010}} - -@article{VydVoo-PRL-09, - Author = {O. A. Vydrov and T. van Voorhis}, - Journal = {Phys. Rev. Lett.}, - Pages = {063004}, - Volume = {103}, - Year = {2009}} - -@article{Wal-TFS-45, - Author = {A. D. Walsh}, - Journal = {Trans. Faraday Soc.}, - Pages = {498}, - Volume = {41}, - Year = {1945}} - -@article{WanGauWul-JCP-08, - Author = {{F. Wang, J. Gauss, and C. van W\"ullen}}, - Journal = {J. Chem. Phys.}, - Pages = {064113}, - Volume = {129}, - Year = {2008}} - -@article{WanPer-PRB-91, - Author = {Y. Wang and J.P. Perdew}, - Journal = {Phys. Rev. B}, - Pages = {13298}, - Volume = {{44}}, - Year = {1991}} - -@article{WanSch-JCP-96, - Author = {S. G. Wang and W. H. E. Schwarz}, - Journal = {J. Chem. Phys.}, - Pages = {4641}, - Volume = {{105}}, - Year = {1996}} - -@article{WanSchSmi-PRA-00, - Author = {J. Wang and H. L. Schmider and V. H. Smith}, - Journal = {Phys. Rev. A}, - Pages = {016501}, - Volume = {62}, - Year = {2000}} - -@article{WanSmi-IJQC-94, - Author = {J. Wang and V. H. Smith}, - Journal = {Int. J. Quantum. Chem.}, - Pages = {147}, - Volume = {49}, - Year = {1994}} - -@article{WanTriSmi-JCP-92, - Author = {J. Wang and A. N. Tripathi and V. H. Smith}, - Journal = {J. Chem. Phys.}, - Pages = {9188}, - Volume = {97}, - Year = {1992}} - -@article{WanTriSmi-JCP-94, - Author = {J. Wang and A. N. Tripathi and V. H. Smith}, - Journal = {J. Chem. Phys.}, - Pages = {4842}, - Volume = {101}, - Year = {1994}} - -@article{WanZie-JCP-04, - Author = {F. Wang and T. Ziegler}, - Journal = {J. Chem. Phys.}, - Pages = {12191}, - Volume = {121}, - Year = {2004}} - -@article{WasBur-PRL-05, - Author = {A. Wasserman and K. Burke}, - Journal = {Phys. Rev. Lett.}, - Pages = {163006}, - Volume = {95}, - Year = {2005}} - -@article{WasMaiBur-PRL-03, - Author = {A. Wasserman and N. T. Maitra and K. Burke}, - Journal = {Phys. Rev. Lett.}, - Pages = {263001}, - Volume = {91}, - Year = {2003}} - -@article{WatKamYamUdaMul-MP-04, - Author = {Noboru Watanabe and Yohei Kamata and Kota Yamauchi and Yasuo Udagawa and Thomas M\"uller}, - Journal = {Mol. Phys.}, - Pages = {649}, - Volume = {102}, - Year = {2004}} - -@article{WeiDelGor-JCP-08, - Author = {M. Weimer and F. Della Sala and A. G\"orling}, - Journal = {J. Chem. Phys.}, - Pages = {144109}, - Title = {Multiconfiguration optimized effective potential method for a density-functional treatment of static correlation}, - Volume = {128}, - Year = {2008}} - -@article{WenBer-JCTC-11, - Author = {Shuhao Wen and Gregory J. O. Beran}, - Journal = {J. Chem. Theory Comput.}, - Pages = {3733}, - Volume = {7}, - Year = {2011}} - -@article{WerKno-JCP-88, - Author = {H.-J. Werner and P. J. Knowles}, - Journal = {J. Chem. Phys.}, - Pages = {5003}, - Volume = {{89}}, - Year = {1988}} - -@article{werner:3144, - Author = {Hans-Joachim Werner and Ernst-Albrecht Reinsch}, - Issue = {6}, - Journal = {The Journal of Chemical Physics}, - Keywords = {CONFIGURATION INTERACTION; ELECTRON CORRELATION; ELECTRONIC STRUCTURE; WAVE FUNCTIONS; DIPOLE MOMENTS; POTENTIAL ENERGY; MOLECULAR MODELS}, - Page = {3144-3156}, - Publisher = {AIP}, - Title = {The self-consistent electron pairs method for multiconfiguration reference state functions}, - Url = {http://link.aip.org/link/?JCP/76/3144/1}, - Volume = {76}, - Year = {1982}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/76/3144/1}} - -@book{Weyl-56, - Address = {New York}, - Author = {H. Weyl}, - Publisher = {Dover}, - Title = {Theory of Groups and Quantum Mechanics}, - Year = {1956}} - -@article{WhiBur-JCP-05, - Author = {Takeyce K. Whittingham and Kieron Burke}, - Journal = {J. Chem. Phys.}, - Number = {13}, - Pages = {134108}, - Title = {Relations between coordinate and potential scaling in the high-density limit}, - Volume = {122}, - Year = {2005}} - -@article{Wig-PR-48, - Author = {E. Wigner}, - Journal = {Phys. Rev.}, - Pages = {1002}, - Volume = {73}, - Year = {1948}} - -@article{WilMouDun-JMS-96, - Author = {A. K. Wilson and T. v. Mourik and T. H. Dunning}, - Journal = {J. Mol. Struct.}, - Pages = {339}, - Volume = {388}, - Year = {1996}} - -@article{WilWooPetDun-JCP-99, - Author = {A.K. Wilson and D.E. Woon and K.A. Peterson and T.H.Dunning}, - Journal = {J. Chem. Phys.}, - Pages = {7667}, - Volume = {110}, - Year = {1999}} - -@article{WodJanRagCor-JPCA-08, - Author = {{M. D. Wodrich, D. F. Jana, P. v. R. Schleyer, and C. Corminboeuf}}, - Journal = {J. Phys. Chem. A}, - Pages = {11495}, - Volume = {112}, - Year = {2008}} - -@article{Wol-PRL-89, - Author = {Wolff, U.}, - Doi = {10.1103/PhysRevLett.62.361}, - Issue = {4}, - Journal = {Phys. Rev. Lett.}, - Numpages = {0}, - Pages = {361--364}, - Publisher = {American Physical Society}, - Title = {{Collective Monte Carlo updating for spin systems}}, - Url = {http://link.aps.org/doi/10.1103/PhysRevLett.62.361}, - Volume = {62}, - Year = {1989}, - Bdsk-Url-1 = {http://link.aps.org/doi/10.1103/PhysRevLett.62.361}, - Bdsk-Url-2 = {https://doi.org/10.1103/PhysRevLett.62.361}} - -@article{wolinski:3647, - Author = {Krzysztof Wolinski and Peter Pulay}, - Journal = {The Journal of Chemical Physics}, - Keywords = {PERTURBATION THEORY; WAVE FUNCTIONS; ELECTRONIC STRUCTURE; DIPOLE MOMENTS; AFFINITY; IONIZATION POTENTIAL; POTENTIAL ENERGY SURFACES; HYDROFLUORIC ACID; FLUORINE; ETHYLENE; OZONE; FORMALDEHYDE; ELECTRON CORRELATION}, - Number = {7}, - Pages = {3647-3659}, - Publisher = {AIP}, - Title = {Generalized M[o-slash]ller--Plesset perturbation theory: Second order results for two-configuration, open-shell excited singlet, and doublet wave functions}, - Url = {http://link.aip.org/link/?JCP/90/3647/1}, - Volume = {90}, - Year = {1989}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/90/3647/1}} - -@article{WooDun-JCP-93, - Author = {D.E. Woon and T.H. Dunning}, - Journal = {J. Chem. Phys.}, - Pages = {1358}, - Volume = {98}, - Year = {1993}} - -@article{WooDun-JCP-94, - Author = {D.E. Woon and T.H. Dunning}, - Journal = {J. Chem. Phys.}, - Pages = {2975}, - Volume = {100}, - Year = {1994}} - -@article{WooDun-JCP-95, - Author = {D.E. Woon and T.H. Dunning}, - Journal = {J. Chem. Phys.}, - Pages = {4572}, - Volume = {103}, - Year = {1995}} - -@article{WouNec-EPJD-14, - Author = {{S. Wouters and D. Van Neck}}, - Journal = {Eur. Phys. J. D}, - Pages = {272}, - Title = {The density matrix renormalization group for ab initio quantum chemistry}, - Volume = {68}, - Year = {2014}} - -@article{WuAyeYan-JCP-03, - Author = {Qin Wu and Paul W. Ayers and Weitao Yang}, - Journal = {J. Chem. Phys.}, - Keywords = {density functional theory; variational techniques; electron affinity; negative ions}, - Number = {6}, - Pages = {2978-2990}, - Publisher = {AIP}, - Title = {Density-functional theory calculations with correct long-range potentials}, - Url = {http://link.aip.org/link/?JCP/119/2978/1}, - Volume = {119}, - Year = {2003}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/119/2978/1}} - -@article{WuCheVoo-JCP-07, - Author = {{Q. Wu, C.-L. Cheng, and T. Van Voorhis}}, - Journal = {J. Chem. Phys.}, - Pages = {164119}, - Title = {Configuration interaction based on constrained density functional theory: A multireference method}, - Volume = {127}, - Year = {2007}} - -@article{WuKadVoo-JCP-09, - Author = {{Q. Wu, B. Kaduk, and T. Van Voorhis}}, - Journal = {J. Chem. Phys.}, - Pages = {034109}, - Volume = {130}, - Year = {2009}} - -@incollection{Wul-INC-10, - Address = {Netherlands}, - Author = {{C. van W\"ullen}}, - Booktitle = {Relativistic Methods for Chemists, Challenges and Advances in Computational Chemistry and Physics 10}, - Editor = {M. Barysz and Y. Ishikawa}, - Pages = {191-214}, - Publisher = {Springer}, - Title = {RELATIVISTIC DENSITY FUNCTIONAL THEORY}, - Year = {2010}} - -@article{WuSha-CPL-99, - Author = {W. Wu and S. Shaik}, - Journal = {Chem. Phys. Lett.}, - Pages = {37}, - Volume = {301}, - Year = {1999}} - -@article{WuShaHib-xx, - Author = {P. Su and J. Wu. and J. Gu and W. Wu and S. Shaik and P. C. Hiberty}, - Journal = {J. Chem. Theory Comput.}, - Pages = {121}, - Volume = {7}, - Year = {2011}} - -@article{WuSonCaoZhaSha-JPCA-02, - Author = {W. Wu and L. Song and Z. Cao and Q. Zhang and S. Shaik}, - Journal = {J. Phys. Chem. A}, - Pages = {2721}, - Volume = {106}, - Year = {2002}} - -@article{WuVarNayLotSco-JCP-01, - Author = {X. Wu and M. C. Vargas and S. Nayak and V. Lotrich and G. Scoles}, - Journal = {J. Chem. Phys.}, - Pages = {8748}, - Volume = {115}, - Year = {2001}} - -@article{WuWuMo-IJQC-98, - Author = {W. Wu and A. Wu and Y. Mo and M. Lin and Q. Zhang}, - Journal = {Int. J. Quantum Chem.}, - Pages = {287}, - Volume = {67}, - Year = {1998}} - -@article{WuYan-JCP-02, - Author = {Q. Wu and W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {515}, - Volume = {116}, - Year = {2002}} - -@article{WuYan-JCP-03, - Author = {Qin Wu and Weitao Yang}, - Journal = {J. Chem. Phys.}, - Number = {6}, - Pages = {2498-2509}, - Title = {A direct optimization method for calculating density functionals and exchange--correlation potentials from electron densities}, - Volume = {118}, - Year = {2003}} - -@article{xantheas:8054, - Author = {Sotiris S. Xantheas and Gregory J. Atchity and Stephen T. Elbert and Klaus Ruedenberg}, - Journal = {The Journal of Chemical Physics}, - Keywords = {OZONE; ELECTRONIC STRUCTURE; POTENTIAL ENERGY; SELF–CONSISTENT FIELD; CONFIGURATION INTERACTION; POTENTIAL ENERGY SURFACES; QUANTUM CHEMISTRY}, - Number = {12}, - Pages = {8054-8069}, - Publisher = {AIP}, - Title = {Potential energy surfaces of ozone. I}, - Url = {http://link.aip.org/link/?JCP/94/8054/1}, - Volume = {94}, - Year = {1991}, - Bdsk-Url-1 = {http://link.aip.org/link/?JCP/94/8054/1}} - -@article{YamKocTen-JCP-07, - Author = {D. Yamaki and H. Koch and S. Ten-no}, - Journal = {J. Chem. Phys.}, - Pages = {144104}, - Volume = {127}, - Year = {2007}} - -@article{YamNakUkaTakYam-IJQC-06, - Author = {S. Yamanaka and K. Nakata and T. Ukai and T. Takada and K. Yamaguchi}, - Journal = {Int. J. Quantum Chem.}, - Pages = {3312}, - Title = {Multireference Density Functional Theory With Orbital-Dependent Correlation Corrections}, - Volume = {106}, - Year = {2006}} - -@article{YanAyeWu-PRL-04, - Author = {Weitao Yang and Paul W. Ayers and Qin Wu}, - Journal = {Phys. Rev. Lett.}, - Pages = {146404}, - Volume = {92}, - Year = {2003}} - -@article{YanCohMor-JCP-12, - Author = {Weitao Yang and Aron J. Cohen and Paula Mori-S\'anchez}, - Journal = {J. Chem. Phys.}, - Pages = {204111}, - Volume = {136}, - Year = {2012}} - -@article{YanFaaBur-JCP-09, - Author = {{Z.-h. Yang, M. van Faassen, and K. Burke}}, - Journal = {J. Chem. Phys.}, - Pages = {114308}, - Volume = {131}, - Year = {2009}} - -@article{YanHarHan-MP-05, - Author = {T. Yanai and R. J. Harrison and N. C. Handy}, - Journal = {Mol. Phys.}, - Pages = {413}, - Volume = {103}, - Year = {2005}} - -@article{Yan-JCP-98, - Author = {W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {10107}, - Title = {Generalized adiabatic connection in density functional theory}, - Volume = {{109}}, - Year = {1998}} - -@article{YanMorCoh-JCP-13, - Author = {W. Yang and P. Mori-S{\'a}nchez and A. J. Cohen}, - Journal = {J. Chem. Phys.}, - Pages = {104114}, - Volume = {139}, - Year = {2013}} - -@article{YanPerKur-PRB-00, - Author = {Yan, Z. and Perdew, J. P. and Kurth, S.}, - Journal = {Phys. Rev. B.}, - Pages = {16430-16439}, - Title = {Density functional for short-range correlation: Accuracy of the random-phase approximation for isoelectronic energy changes}, - Volume = {61}, - Year = {2000}} - -@article{YanTewHan-CPL-04, - Author = {Takeshi Yanai and David P. Tew and Nicholas C. Handy}, - Journal = {Chem. Phys. Lett.}, - Pages = {51}, - Volume = {393}, - Year = {2004}} - -@article{YanWu-PRL-02, - Author = {Weitao Yang and Qin Wu}, - Journal = {Phys. Rev. Lett.}, - Pages = {143002}, - Title = {Direct Method for Optimized Effective Potentials in Density-Functional Theory}, - Volume = {89}, - Year = {2002}} - -@article{YanZhaAye-PRL-00, - Author = {Weitao Yang and Yingkai Zhang and Paul W. Ayers}, - Journal = {Phys. Rev. Lett.}, - Pages = {5172}, - Volume = {84}, - Year = {2000}} - -@article{Yar-CPL-81, - Author = {D. R. Yarkony}, - Journal = {Chem. Phys. Lett.}, - Pages = {634}, - Volume = {77}, - Year = {1981}} - -@article{Yas-PRL-02, - Author = {Koji Yasuda}, - Eid = {053001}, - Journal = {Physical Review Letters}, - Keywords = {density functional theory; electron density; electron correlations; Schrodinger equation; scaling phenomena; electron gas}, - Number = {5}, - Numpages = {4}, - Pages = {053001}, - Publisher = {APS}, - Title = {Local Approximation of the Correlation Energy Functional in the Density Matrix Functional Theory}, - Url = {http://link.aps.org/abstract/PRL/v88/e053001}, - Volume = {88}, - Year = {2002}, - Bdsk-Url-1 = {http://link.aps.org/abstract/PRL/v88/e053001}} - -@article{YeaJor-JCP-79, - Author = {D. L. Yeager and P. J{\o}rgensen}, - Journal = {J. Chem. Phys.}, - Pages = {755}, - Volume = {{71}}, - Year = {1979}} - -@article{YinSuCheShaWu-JCTC-12, - Author = {F. Ying and P. Su and Z. Chen and S. Shaik and W. Wu}, - Journal = {J. Chem. Theory Comput.}, - Pages = {1608}, - Volume = {8}, - Year = {2012}} - -@article{Yu-IJQC-13, - Author = {F. Yu}, - Journal = {Int. J. Quantum Chem.}, - Pages = {2355}, - Volume = {113}, - Year = {2013}} - -@article{ZahLeaGor-JCP-13, - Author = {F. Zahariev and S. S. Leang and M. S. Gordon}, - Journal = {J. Chem. Phys.}, - Pages = {244108}, - Volume = {138}, - Year = {2013}} - -@book{ZalPapMezLes-BOOK-11, - Address = {Netherlands}, - Editor = {R. Zalesny and M. G. Papadopoulos and P. G. Mezey and J. Leszczynski}, - Publisher = {Springer}, - Series = {Challenges and Advances in Computational Chemistry and Physics Vol. 13}, - Title = {Linear-Scaling Techniques in Computational Chemistry and Physics}, - Year = {2011}} - -@article{ZanSov-PRA-80, - Author = {A. Zangwill and P. Soven}, - Journal = {Phys. Rev. A}, - Pages = {1561}, - Volume = {21}, - Year = {1980}} - -@article{ZapLupTou-JCP-19, - Author = {F. Zapata and E. Luppi and J. Toulouse}, - Doi = {10.1063/1.5096037}, - Journal = {J. Chem. Phys.}, - Pages = {234104}, - Title = {Linear-response range-separated density-functional theory for atomic photoexcitation and photoionization spectra}, - Volume = {150}, - Year = {2019}, - Bdsk-Url-1 = {https://doi.org/10.1063/1.5096037}} - -@misc{ZapLupTou-JJJ-XX-note, - Note = {Contrary to our Fig. \ref{Hespectra}a, the TDLDA spectrum of the He atom shown in Fig. 6 of Ref.~\onlinecite{WasMaiBur-PRL-03} has a larger maximum than the LDA spectrum. This discrepancy is due to the fact that the TDLDA spectrum shown in Ref.~\onlinecite{WasMaiBur-PRL-03} comes in fact from Ref.~\onlinecite{SteDecGor-JCP-01} where it was calculated by replacing the LDA 1s orbital energy by the opposite of the exact ionization energy. We have checked that this results not only in an energy shift of the spectrum but also to larger oscillator strengths. The true TDLDA spectrum of the He atom is thus the one shown in the present Fig. \ref{Hespectra}a.}} - -@article{ZarKoh-PRB-76, - Author = {E. Zaremba and W. Kohn}, - Journal = {Phys. Rev. B}, - Pages = {2270}, - Volume = {13}, - Year = {1976}} - -@article{ZecGorMorBac-PRB-04, - Author = {Lorenzo Zecca and Paola Gori-Giorgi and Saverio Moroni and Giovanni B. Bachelet}, - Journal = {Phys. Rev. B}, - Keywords = {density functional theory; Monte Carlo methods; ground states; electron gas; electron density; electron correlations}, - Number = {20}, - Pages = {205127}, - Publisher = {APS}, - Title = {Local density functional for the short-range part of the electron-electron interaction}, - Volume = {70}, - Year = {2004}} - -@article{ZeiMea-MP-77, - Author = {G. D. Zeiss and W. J. Meath}, - Journal = {Mol. Phys.}, - Pages = {1155}, - Volume = {33}, - Year = {1977}} - -@article{ZhaBur-PRA-04, - Author = {F. Zhang and K. Burke}, - Journal = {Phys. Rev. A}, - Pages = {052510}, - Volume = {69}, - Year = {2004}} - -@article{ZhaLuoXu-JCP-10b, - Author = {I. Y. Zhang and Y. Luo and X. Xu}, - Journal = {J. Chem. Phys.}, - Pages = {104105}, - Volume = {133}, - Year = {2010}} - -@article{ZhaLuoXu-JCP-10, - Author = {I. Y. Zhang and Y. Luo and X. Xu}, - Journal = {J. Chem. Phys.}, - Pages = {194105}, - Volume = {132}, - Year = {2010}} - -@article{ZhaLynTru-JPCA-04, - Author = {Y. Zhao and B. J. Lynch and D. G. Truhlar}, - Journal = {J. Phys. Chem. A}, - Pages = {4786}, - Volume = {108}, - Year = {2004}} - -@article{ZhaLynTru-PCCP-05, - Author = {Y. Zhao and B. J. Lynch and D. G. Truhlar}, - Journal = {Phys. Chem. Chem. Phys.}, - Pages = {43}, - Volume = {7}, - Year = {2005}} - -@article{ZhaPar-PRA-92, - Author = {Q. Zhao and R. G. Parr}, - Journal = {Phys. Rev. A.}, - Pages = {2337}, - Volume = {{46}}, - Year = {1992}} - -@article{ZhaSchTru-JCTC-06, - Author = {Y. Zhao and N. E. Schultz and D. G. Truhlar}, - Journal = {J. Chem. Theory Comput.}, - Pages = {364}, - Volume = {2}, - Year = {2006}} - -@article{ZhaSteYan-JCP-13, - Abstract = {We present a dynamical second-order kernel for the Bethe-Salpeter equation to calculate electronic excitation energies. The derivation takes explicitly the functional derivative of the exact second-order self energy with respect to the one-particle Green's function. It includes naturally a frequency dependence, going beyond the adiabatic approximation. Perturbative calculations under the Tamm-Dancoff approximation, using the configuration interaction singles (CIS) eigenvectors, reveal an appreciable improvement over CIS, time-dependent Hartree-Fock, and adiabatic time-dependent density functional theory results. The perturbative results also compare well with equation-of-motion coupled-cluster and experimental results.}, - Author = {Zhang, Du and Steinmann, Stephan N and Yang, Weitao}, - Journal = {J. Chem. Phys.}, - Month = oct, - Number = {15}, - Pages = {154109}, - Pmid = {24160502}, - Publisher = {American Institute of Physics}, - Title = {{Dynamical second-order Bethe-Salpeter equation kernel: A method for electronic excitation beyond the adiabatic approximation.}}, - Volume = {139}, - Year = {2013}} - -@article{ZhaSuBreAdaXu-JCP-12, - Author = {I. Y. Zhang and N. Q. Su and E. A. G. Br\'emond and C. Adamo}, - Journal = {J. Chem. Phys.}, - Pages = {174103}, - Volume = {136}, - Year = {2012}} - -@article{ZhaTru-JCTC-07, - Author = {Y. Zhao and D. G. Truhlar}, - Journal = {J. Chem. Theory Comput.}, - Pages = {289}, - Title = {Density Functionals for Noncovalent Interaction Energies of Biological Importance}, - Volume = {3}, - Year = {2007}} - -@article{ZhaTru-TCA-08, - Author = {Y. Zhao and D. G. Truhlar}, - Journal = {Theor. Chem. Acc.}, - Pages = {215}, - Volume = {120}, - Year = {2008}} - -@article{ZhaWuXu-CC-10, - Author = {I. Y. Zhang and J. Wu and X. Xu}, - Journal = {Chem. Commun.}, - Pages = {3057}, - Volume = {46}, - Year = {2010}} - -@article{ZhaXuGod-PNAS-09, - Author = {{Y. Zhang, X. Xu and W. A. Goddard III}}, - Journal = {Proc. Natl. Acad. Sci. U.S.A.}, - Pages = {4963}, - Volume = {106}, - Year = {2009}} - -@article{ZhaXuGod-PNAS-09_fr, - Author = {{Y. Zhang, X. Xu et W. A. Goddard III}}, - Journal = {Proc. Natl. Acad. Sci. U.S.A.}, - Pages = {4963}, - Volume = {106}, - Year = {2009}} - -@article{ZhaXu-IRPC-11, - Author = {I. Y. Zhang and X. Xu}, - Journal = {Int. Rev. Phys. Chem.}, - Pages = {115}, - Volume = {30}, - Year = {2011}} - -@article{ZhaXu-JPCL-13, - Author = {I. Y. Zhang and X. Xu}, - Journal = {J. Phys. Chem. Lett.}, - Pages = {1669}, - Volume = {4}, - Year = {2013}} - -@article{ZhaXuJunGod-PNAS-11, - Author = {{I. Y. Zhang, X. Xu, Y. Jung, and W. A. Goddard III}}, - Journal = {Proc. Natl. Acad. Sci. U.S.A.}, - Pages = {19896}, - Volume = {108}, - Year = {2011}} - -@article{ZhaYan-JCP-98, - Author = {Y. Zhang and W. Yang}, - Journal = {J. Chem. Phys.}, - Pages = {2604}, - Volume = {109}, - Year = {1998}} - -@article{ZheZhaTru-JCTC-07, - Author = {J. Zheng and Y. Zhao and D. G. Truhlar}, - Journal = {J. Chem. Theory Comput.}, - Pages = {569}, - Volume = {3}, - Year = {2007}} - -@article{ZheZhaTru-JCTC-09, - Author = {J. Zheng and Y. Zhao and D. G. Truhlar}, - Journal = {J. Chem. Theory Comput.}, - Pages = {808}, - Volume = {5}, - Year = {2009}} - -@article{ZhoChu-PRA-09, - Author = {Z. Zhou and S.-I. Chu}, - Journal = {Phys. Rev. A}, - Pages = {053412}, - Volume = {79}, - Year = {2009}} - -@article{ZhuTouSavAng-JCP-10, - Author = {Wuming Zhu and Julien Toulouse and Andreas Savin and J\'anos G. \'Angy\'an}, - Journal = {J. Chem. Phys.}, - Pages = {244108}, - Title = {Range-separated density-functional theory with random phase approximation applied to noncovalent intermolecular interactions}, - Volume = {132}, - Year = {2010}} - -@misc{ZhuTouSavAng-JJJ-XX, - Author = {W. Zhu and J. Toulouse and A. Savin and J. G. \'Angy\'an}, - Note = {unpublished}} - -@article{ZieCio-PA-05, - Author = {P. Ziesche and J. Cioslowski}, - Journal = {Physica A}, - Year = {to appear}} - -@article{Zie-JPC-80, - Author = {P. Ziesche}, - Journal = {J. Phys. C}, - Pages = {3625}, - Volume = {13}, - Year = {1980}} - -@article{ZieRauBae-TCA-77, - Author = {T. Ziegler and A. Rauk and E. J. Baerends}, - Journal = {Theor. Chem. Acc.}, - Pages = {261}, - Volume = {43}, - Year = {1977}} - -@article{ZieSetKryAutWan-JCP-09, - Author = {T. Ziegler and M. Seth and M. Krykunov and J. Autschbach and F. Wang}, - Journal = {J. Chem. Phys.}, - Pages = {154102}, - Volume = {130}, - Year = {2009}} - -@article{ZimParKou-JCP-04, - Author = {U. Zimmerli and M. Parrinello and P. Koumoutsakos}, - Journal = {J. Chem. Phys.}, - Pages = {2693}, - Volume = {120}, - Year = {2004}} - -@article{ZimTouZhaMusUmr-JCP-09, - Author = {P. M. Zimmerman and J. Toulouse and Z. Zhang and C. B. Musgrave and C. J. Umrigar}, - Journal = {J. Chem. Phys.}, - Pages = {124103}, - Title = {Excited states of methylene from quantum Monte Carlo}, - Volume = {131}, - Year = {2009}} - -@article{ZucPodMosJezSza-JCP-08, - Author = {P. S. Zuchowski and R. Podeszwa and R. Moszynski and B. Jeziorski and K. Szalewicz}, - Journal = {J. Chem. Phys.}, - Pages = {084101}, - Title = {{Symmetry-adapted perturbation theory utilizing density functional description of monomers for high-spin open-shell complexes}}, - Volume = {129}, - Year = {2008}} diff --git a/Revised_Manuscript/data/C2/DFT_avdzE_relat-eps-converted-to.pdf b/Revised_Manuscript/data/C2/DFT_avdzE_relat-eps-converted-to.pdf deleted file mode 100644 index 66a8e4e2f3a20e43bfd23558222455330acdc6c7..0000000000000000000000000000000000000000 GIT binary patch literal 0 HcmV?d00001 literal 13914 zcmb_@2Ut_f_OCRNfCz#hC=hxlB-GH9-g^fD1BBiQMLLQi9Rx%H>4-Fuj(~#nj`ZF^ zdQ*CRJ08!uo^$X2|K9t)yYppd_L?(v?_x!@BCMClO_MK%&56p643)&s zV%E<>#d^R_kb7Z^Ltk2)1Fq~wUZE+0Uo-3O2(-N3*|A)7pHQ`NwnpFc1zPem4wyK z8V*Jk=W5~YL_tvso;#Af6p0b3TU<5g*ML}!OXkHoL z_i5aQ$_^Q4atYyb<17jx9a%(8-`>g6fi0hZbbj>xzDu8Y#57lQ1y|4XbL!E|G-@nq zv%v`btilvCKNbf2TR7T&tD&RDEH7@W^GZ!s$t5-vd{@)Sst7ZWGuc?R;Ns__GuJ(Q z)f;DaZug=a>w3jrR)xaRPJIPayUNtNO~Osb2T49x!aW)VNJNyp6bZ 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