2012
DOI: 10.1088/1367-2630/14/1/013032
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The Kadanoff–Baym approach to double excitations in finite systems

Abstract: We benchmark many-body perturbation theory by studying neutral, as well as non-neutral, excitations of finite lattice systems. The neutral excitation spectra are obtained by time-propagating the Kadanoff-Baym equations in the Hartree-Fock and the second Born approximations. Our method is equivalent to solving the Bethe-Salpeter equation with a high-level kernel while respecting self-consistency, which guarantees the fulfillment of a frequency sum rule. As a result, we find that a time-local method, such as Har… Show more

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Cited by 37 publications
(51 citation statements)
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“…To answer we have to find the diagrammatic structure encoded in the kernel of the BSE. where L 0 (12; 34) = G(1, 4)G(2, 3) and the fourpoint reducible kernel K is given by K(12; 34) = −iδΣ(1, 3)/δG (4,2). The variation of the Green's function is related to the two-particle Green's function and therefore L is related to the two-particle excitation spectrum.…”
Section: Examplesmentioning
confidence: 99%
“…To answer we have to find the diagrammatic structure encoded in the kernel of the BSE. where L 0 (12; 34) = G(1, 4)G(2, 3) and the fourpoint reducible kernel K is given by K(12; 34) = −iδΣ(1, 3)/δG (4,2). The variation of the Green's function is related to the two-particle Green's function and therefore L is related to the two-particle excitation spectrum.…”
Section: Examplesmentioning
confidence: 99%
“…with |X being the eigenstates ofĤ 2 (having energy E X ) and c X = X|gs denoting the expansion coefficients with respect to the ground state |gs ofĤ 0 . In contrast to the HF approximation, a second-order self-energy (as 2B) has the ability to describe double excitations, see [22]. For this reason, the 2B+GKBA calculations capture the transition ω AD and, accordingly, also ω CD .…”
Section: Discussionmentioning
confidence: 99%
“…We mention that the 2B approximation has been successfully applied to equilibrium spectral properties [49] and total energies [50] of molecular systems. Comparisons against numerically accurate real-time simulations of 1D systems [18,51] and weakly correlated model nanostructures of different geometries [29,30,39,[52][53][54][55][56] indicate that the 2B approximation remains accurate even out of equilibrium. The last term I Auger can be written as in Eq.…”
Section: A Negf Equationsmentioning
confidence: 99%