Merge branch 'master' of https://git.irsamc.ups-tlse.fr/loos/sfBSE

Manuscript/sfBSE.tex

@@ -822,6 +822,8 @@ Finally, both SF-ADC(2)-x and SF-ADC(3) yield excitation energies very close to
 			SF-TD-BLYP\fnm[1]		&	(0.002)	&	3.210(1.000)	&	3.210(1.000)	&	6.691(1.000)	&	7.598(0.013)	\\
 			SF-TD-B3LYP\fnm[1]		&	(0.001)	&	3.332(1.839)	&	4.275(0.164)	&	6.864(1.000)	&	7.762(0.006)	\\	
 			\alert{SF-TD-CAM-B3LYP} &	(0.001) &	3.186(1.960)	&	4.554(0.043)	&	7.020(1.000)	&	7.933(0.008)	\\
+			\alert{SF-TD-$\omega$B97X-D} & (0.006) & 3.337(1.867) & 4.717(0.147)	& 7.076(1.000) & 8.247(0.040)\\
+			\alert{SF-TD-LC-$\omega$PBE08} & (0.014) & 3.434(1.720) &5.904(0.287)& 7.088(1.000) & 9.471(0.073) \\
 			SF-TD-BH\&HLYP\fnm[1]	&	(0.000)	&	2.874(1.981)	&	4.922(0.023)	&	7.112(1.000)	&	8.188(0.002)	\\
 			SF-CIS\fnm[2]			&	(0.002)	&	2.111(2.000)	&	6.036(0.014)	&	7.480(1.000)	&	8.945(0.006)	\\
 			SF-BSE@{\GOWO}			&	(0.004)	&	2.399(1.999)	&	6.191(0.023)	&	7.792(1.000)	&	9.373(0.013)	\\
@@ -987,6 +989,8 @@ This issue does not appear at the SF-BSE, SF-ADC, and SF-EOM-SF-CCSD levels.
 			\hline
 			SF-TD-B3LYP\fnm[1] 		&	$1.750$	&	$2.260$	&	$4.094$	\\
 			\alert{SF-TD-CAM-B3LYP} &	$1.790$ &	$2.379$ &	$4.238$ \\
+			\alert{SF-TD-$\omega$B97X-D} & $1.771$ & $2.366$ & $4.212$ \\
+			\alert{SF-TD-LC-$\omega$PBE08} & $1.941$ & $2.464$ & $4.428$  \\
 			SF-TD-BH\&HLYP\fnm[1] 	&	$1.583$	&	$2.813$	&	$4.528$	\\
 			SF-CIS\fnm[2]			&	$1.521$	&	$3.836$	&	$5.499$	\\
 			EOM-SF-CCSD\fnm[3]		&	$1.654$	&	$3.416$	&	$4.360$	\\
@@ -1020,6 +1024,8 @@ This issue does not appear at the SF-BSE, SF-ADC, and SF-EOM-SF-CCSD levels.
 			\hline
 			SF-TD-B3LYP\fnm[1]		&	$-0.020$	&	$0.547$	&	$0.486$	\\
 			\alert{SF-TD-CAM-B3LYP} &	$0.012$		&	$0.677$ &	$0.595$ \\
+			\alert{SF-TD-$\omega$B97X-D} & $0.005$ & $0.673$ & $0.592$  \\
+			\alert{SF-TD-LC-$\omega$PBE08} & $0.062$ & $0.663$ & $0.570$   \\
 			SF-TD-BH\&HLYP\fnm[1]	&	$0.048$		&	$1.465$	&	$1.282$	\\
 			SF-CIS\fnm[2]			&	$0.317$		&	$3.125$	&	$2.650$	\\
 			EOM-SF-CCSD\fnm[3]		&	$0.369$		&	$1.824$	&	$2.143$	\\