From b92deb622e318d8c90c56394b2696f52e6d0815f Mon Sep 17 00:00:00 2001 From: Antoine MARIE Date: Mon, 27 Mar 2023 22:32:26 +0200 Subject: [PATCH] add footer, work on second line of boxes --- Poster/main.tex | 35 +++++++++++++++++------------------ Poster/upfolding.pdf | Bin 47403 -> 47347 bytes 2 files changed, 17 insertions(+), 18 deletions(-) diff --git a/Poster/main.tex b/Poster/main.tex index 7328eab..d3adb76 100644 --- a/Poster/main.tex +++ b/Poster/main.tex @@ -22,6 +22,7 @@ \definecolor{fooyellow}{RGB}{234,180,0} \definecolor{lavender}{rgb}{0.71, 0.49, 0.86} \definecolor{inchworm}{rgb}{0.7, 0.93, 0.36} +\definecolor{footer}{cmyk}{0.739,0.288,0,0.278} \newcommand{\violet}[1]{\textcolor{violet}{#1}} \newcommand{\orange}[1]{\textcolor{orange}{#1}} \newcommand{\purple}[1]{\textcolor{purple}{#1}} @@ -151,17 +152,17 @@ \column{0.5} \block{Similarity Renormalization Group (SRG)}{ \begin{minipage}{0.49\linewidth} - The pillar of the SRG formalism is the flow equation + SRG flow equation \begin{equation} \label{eq:flowEquation} \dv{\boldsymbol{H}(s)}{s} = \comm{\boldsymbol{\eta}(s)}{\boldsymbol{H}(s)} \end{equation} - with the similarity transformed Hamiltonian + Similarity transformed Hamiltonian \begin{equation} \label{eq:SRG_Ham} \boldsymbol{H}(s) = \boldsymbol{U}(s) \, \boldsymbol{H} \, \boldsymbol{U}^\dagger(s) \end{equation} - In this work, we use Wegner's generator + Wegner generator %\begin{equation} % \boldsymbol{\eta}(s) = \dv{\boldsymbol{U}(s)}{s} \boldsymbol{U}^\dagger(s) = - \boldsymbol{\eta}^\dag(s) %\end{equation} @@ -172,7 +173,7 @@ \hfill\vline\hfill \begin{minipage}{0.49\linewidth} \begin{tikzfigure} - \includegraphics[width=0.9\textwidth]{SRGMatrix} + \includegraphics[width=1.1\textwidth]{SRGMatrix} \end{tikzfigure} \end{minipage} } @@ -188,18 +189,17 @@ \column{0.65} \block{SRG-$GW$} { - \begin{minipage}{0.575\linewidth} + \begin{minipage}{0.6\linewidth} \begin{equation*} \begin{split} - &\blue{\widetilde{\boldsymbol{F}}_{pq}}(s) = \delta_{pq} \blue{\epsilon^{\text{HF}}_{p}} + \sum_{r\nu} \frac{\Delta_{pr}^{\nu} + \Delta_{qr}^{\nu}}{(\Delta_{pr}^{\nu})^2 + (\Delta_{qr}^{\nu})^2 } \red{W_{pr}^{\nu}} \red{W_{qr}^{\nu}} \qty[1 - e^{-((\Delta_{pr}^{\nu})^2+(\Delta_{qr}^{\nu})^2) s} ] \\ - &\qq{with} \Delta_{pr}^{\nu} = \teal{\epsilon^{GW}_{p}} - \teal{\epsilon^{GW}_{r}} \pm \orange{\Omega_{\nu}} \\ + \blue{\widetilde{\boldsymbol{F}}_{pq}}(s) &= \delta_{pq} \blue{\epsilon^{\text{HF}}_{p}} + \sum_{r\nu} \frac{\Delta_{pr}^{\nu} + \Delta_{qr}^{\nu}}{(\Delta_{pr}^{\nu})^2 + (\Delta_{qr}^{\nu})^2 } \red{W_{pr}^{\nu}} \red{W_{qr}^{\nu}} \qty[1 - e^{-((\Delta_{pr}^{\nu})^2+(\Delta_{qr}^{\nu})^2) s} ] \\ + \Delta_{pr}^{\nu} &= \teal{\epsilon^{GW}_{p}} - \teal{\epsilon^{GW}_{r}} \pm \orange{\Omega_{\nu}} \\ \\ - &\violet{\widetilde{\Sigma}_{pq}^{\SRGGW}}(\omega;s) = \\ - &\sum_{i\nu} \frac{\red{W_{pi}^{\nu}} \red{W_{qi}^{\nu}}e^{-((\Delta_{pi}^{\nu})^2+(\Delta_{qi}^{\nu})^2) s}}{\omega - \teal{\epsilon^{GW}_{i}} + \orange{\Omega_{\nu}}} + \sum_{a\nu} \frac{\red{W_{pa}^{\nu}} \red{W_{qa}^{\nu}}e^{-((\Delta_{pa}^{\nu})^2+(\Delta_{qa}^{\nu})^2) s}}{\omega - \teal{\epsilon^{GW}_{a}} - \orange{\Omega_{\nu}}} + \violet{\widetilde{\Sigma}_{pq}^{\SRGGW}} &= \sum_{i\nu} \frac{e^{-(\Delta_{pi}^{\nu})^2 s}\red{W_{pi}^{\nu}} \red{W_{qi}^{\nu}}e^{-(\Delta_{qi}^{\nu})^2 s}}{\omega - \teal{\epsilon^{GW}_{i}} + \orange{\Omega_{\nu}}} + \sum_{a\nu} \frac{e^{-(\Delta_{pa}^{\nu})^2 s}\red{W_{pa}^{\nu}} \red{W_{qa}^{\nu}}e^{-(\Delta_{qa}^{\nu})^2 s}}{\omega - \teal{\epsilon^{GW}_{a}} - \orange{\Omega_{\nu}}} \end{split} \end{equation*} \end{minipage} - \begin{minipage}{0.425\linewidth} + \begin{minipage}{0.4\linewidth} \begin{tikzfigure} \includegraphics[width=\textwidth]{fig1.pdf} \end{tikzfigure} @@ -210,8 +210,8 @@ \block{Functional form of the qs$GW$ and SRG-qs$GW$} { - \begin{minipage}[t]{0.275\linewidth} - \vspace{2.5cm} + \begin{minipage}[t]{0.24\linewidth} + \vspace{3cm} \begin{equation*} \begin{split} &\boldsymbol{\Sigma}^{\text{qs}GW}_{pq}(\eta) = \\ @@ -221,14 +221,14 @@ \end{equation*} \end{minipage} \begin{adjustbox}{valign=t} - \begin{minipage}[t]{0.45\linewidth} + \begin{minipage}[t]{0.5\linewidth} \begin{tikzfigure} - \includegraphics[width=0.8\textwidth]{fig2.pdf} + \includegraphics[width=0.82\textwidth]{fig2.pdf} \end{tikzfigure} \end{minipage} \end{adjustbox} - \begin{minipage}[t]{0.275\linewidth} - \vspace{2.5cm} + \begin{minipage}[t]{0.26\linewidth} + \vspace{3cm} \begin{equation*} \begin{split} &\boldsymbol{\Sigma}^{\text{SRG-qs}GW}_{pq}(s) = \\ @@ -270,7 +270,6 @@ This project has received funding from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (Grant agreement No. 863481).} \end{columns} -\node [above right,outer sep=0pt,minimum width=\paperwidth,align=center,draw,fill=blue!30] at (bottomleft) {Blabla}; - +\node [above right,outer sep=0pt,minimum width=\paperwidth,align=left,draw,fill=footer] at (bottomleft) {\Large \textcolor{white}{\textbf{amarie@irsamc.ups-tlse.fr \hspace{50cm} arXiv:2303.05984}} }; \end{document} diff --git a/Poster/upfolding.pdf b/Poster/upfolding.pdf index c1ee33f46cca24dacbb432312005a88ff418efc2..6861aa716a544be8fd58ba4119eda8bdc3ed14bf 100644 GIT binary patch delta 1735 zcmV;&1~~bv@&fbm0+1vEF*uW71}J~6SWR!-HW0o0SMXHW2Tk}j{J1uV4fNDa4D?X+ z5V%fKz;@lVK>PFiC{g^7rCsl?0o#&Bqao+<&EwEgd=*mMT*w1gg}+iL;R0Ffg(Qwa z+&y0WCE#)+M!yS5CI%M&ie$!*A{CiUHcSD&f6b9TA~^ZzrFzZ#moInI5ZQmA6d7lQ zx5S3i#1!F0{%!B?9-F~F-ZYU{#+aiIK2lKW%A|}*@qfI%cz11`h!mZ6;`WQkKH25= zck%1x_0?~;Kdr?5a9cw6Um@_WCN<=&hMLw+lqHz}SYTM6dVGu_Z>+GI6au~mpLtPL zT5QC?{O8*i86^=i;0B?+)9ZiG%ud;7#O8g%=H0c5!cp`lB)>o*O_GeyPWqdA&KOQf zH^?o5E}+W^4>jYRI1(~NF|CXtWBFLf3SckbLXmL5k{XKEY{4}-WuFm=Usm8!nrs5# zwRm+=mv~Lt4mI6l@xlvpBEh!Ma*>qx`?-~UT56q-RUdQ#)tKliv1WhK%&9(#@irP_ zYuSniaZ&D9jmi5#l<#r->BM?>7R$+4bBe*dX}zPc3@}OB!~k@iz}YGL?5%h1*5p}z z+vIN_bg?Ko;h|=HEPtIL8TDJ&JL-x}JW%i1>4bXUi&qzQiPx0vx%GY;!4B2?K5k{7 zmRjdy)dyXz_tS}myiw@tJw3dy_y3vz0QjWnS)*Uy2r1n0Fs7bO^rmmfKAepKrEE3x zIJMb`M%+R%#%K;NS$Ldvq)w?sVy&??c#53#WD1tOJh5b}>zLk=<=9LD?R#_tNevst}DyKY@ocj~hfYJ{Ey52Hu-H4?LY(u5pV6lJ27|oS-)zZ+e7+cyEW1-!U zq*hhZ;W>Jbl5ANwJI$P{VKV2cq2XLHww$ZR%(;?a;atICjdRO0?fMD+z_ES6jFk3A zF!D9W_7`kLk8^;kqeshA^a>+8f0!;fDvZ~=KcBwP#;JbqIlmpC=V*rDAVbR{JZ>4w z0;aQ^O{ag%vc{5v3)WW)M|4J3a>oxFao$m?qlXQoopWI(sP&|^?xbH zxS0W(H78Z7%uI!I4^UpFNrK{#`QWyC zw#g~`j9j|^?^XR8gvi*rU)yc>Yux}V{aO>scc=;XY@2?bL~Gu<{ttp2*R8V-25+k^ zH!?CXH!?XZFfu1FFefPrFHLV`L}7GgASgsSGB7eTFf%eYGBPkXGC3&sMbY=7af%wpICO5r!qzfn8kZrs2-hG8f*^>E zy{oaXw$=NK!~Hz?l75NO6b&>XKQd9HZsl<&s9}sLMkp}B3@xh48G@A=u{*JbM>Mg*A`8Ho;uqAJrsLb zq}km9Nt$j8v_HR;EK8I}p2^HCkcn-YqD1oJC(2TM7E;_@$s<=q|D{mE1+dl&2^fQT zc)t2ekjkCNdRG!m3@H8;NlbqVR75mIFdO*#xmbEn#zBf`0IfwUp2d}+0YQH`*Mv_@ z=rkCoLrB6ja{bH){UYkhcbk*@=%qTaxcYwob72^I#7#ZyDJ0t5>e(E|p;lYwZ>R=9s=rJ|D~@#`R5 zN`p-Scx${mtLu2p-cHTkQ{zQ1%$We&ik6F@yg!VsqQjwed8~S)t59V}N5C4F%6`Q^ zAFKE^R~+Jw0m+w5tC7%pV;EA)diG`f1+3#NfeHzE5QF)qtV88Z5y6{Vtc zkae&_#;f|WSw+3k6*PZ}!&CG4)GBfYWYpi9bqG0V;t|#ZDMuyWdGABgPR2T2L5kgpB8KDoRBs zJ1;j;(kriAFH4`=+D~sVI!w6G_hf@ea-wVWVZ-;LRCIri_}(k8d@n1X>e8F* zmFJi9#)|RF?TFXwPQu?;AwOCeqxSc!BxL6egHm@&Rrn+hZA0DuwsrEU6BecVyxzO= zgv{sse0bM;UTLbORPDsRTH59c2dB`DTaOB7w9Fyk0-P0yXRUO@h#pnq! zsSO}!5nC~$6BMMx1gRK{Qqjr9_{YnQj@SP@etr4)bTfZZ^tNevQbtMhYg^eb729f^`N!H&;V*3c&};y zZ2%>a(I&b!pG6>squsJe4ESJDXUb+X)P{IzW4C_3DmdyZhmf09ibgvZ@4>8}fkCP>&||82G&PqtK*igU zv9N|bwZX=)1nLMbcus^mfQmZwDOCZ`N7vJy@`MxAmG+baX`*7Zrw}m8z-f;}iU^d^ zp0a<5i`fdOS#wgwp7s{Mx&?rZHZkbppG-V#8lZB%&&HB6%NOczh9&Y<%>=Q9rJ~VJ zJEvl)O)tJ1F*Y`B9ai!cApNv@<{qBKQ@ z66EJf)F@hc+zATkqK^&+=wXO5DyX7{y0dBgH9Xrzn_e!Wxi_b1%iDRh?eki`?B(l0 sz8&TJC-xD>nE3IP-!J_EP*o543T19&bCb}x7z;NrGB*k(B}Gq03jU2%8~^|S