From 12608e70591e158a53f0128bc86cf3dbab884657 Mon Sep 17 00:00:00 2001 From: Pierre-Francois Loos Date: Tue, 26 May 2020 12:24:30 +0200 Subject: [PATCH] Updates from Overleaf --- BSEdyn.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/BSEdyn.tex b/BSEdyn.tex index 194a1b3..96e1dcd 100644 --- a/BSEdyn.tex +++ b/BSEdyn.tex @@ -376,7 +376,7 @@ In the following, $i$ and $j$ are occupied orbitals, $a$ and $b$ are unoccupied %\titou{namely $GW$ quasiparticle energies and input Hartree-Fock molecular orbitals in the present study. (T2: shall we really mention this here?)} After projecting onto $\phi_a^*(\bx_1) \phi_i(\bx_{1'})$, one gets \begin{multline} - \int d\bx_1 d\bx_{1'} \; \phi_a^*(\bx_1) \phi_i(\bx_{1'}) L_0(\bx_1,3;\bx_{1'},4; \Oms) + \int d\bx_1 d\bx_{1'} \; \phi_a^*(\bx_1) \phi_i(\bx_{1'}) L_0(\bx_1,4;\bx_{1'},3; \Oms) \\ = \frac{ \phi_a^*(\bx_3) \phi_i(\bx_4) e^{i \Oms t^{34} }} { \Oms - ( \e{a} - \e{i} ) + i \eta }