Generalization of the Hartree-Fock-Bogoliubov theory: one and two quasiparticle excitations

dc.creatorTommasini, Paolo
dc.creatorde Passos, E. J. V.
dc.creatorPires, M. O. C.
dc.creatorPiza, A. F. R. de Toledo
dc.date2003-07-30
dc.date.accessioned2026-07-07T02:52:40Z
dc.date.available2026-07-07T02:52:40Z
dc.descriptionWe present a generalization of the Hartree-Fock Bogoliubov (HFB) theory in which the coupling between one and two quasi-particles is taken into account.This is done by writing the excitation operators as linear combinations of one and two HFB quasi-particles. The excitation energies and the quasi-particle amplitudes are given by generalized Bogoliubov equations. The excitation spectrum has two branches. The first one is a discrete branch which is gapless and has a phonon character at large wave-length and, contrarily to HFB, is always stable. This branch is detached from a continuum branch whose threshold, at fixed total momentum, coincides with the two quasi-particle threshold of the HFB theory. The gap between these two branches at P=0 is equal to two times the HFB gap, which then provides for the relevant energy scale. We also give numerical results for a specific case.
dc.description27 pages, 3 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0307745
dc.identifierhttp://arxiv.org/abs/cond-mat/0307745
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/21926
dc.subjectSoft Condensed Matter
dc.titleGeneralization of the Hartree-Fock-Bogoliubov theory: one and two quasiparticle excitations
dc.typetext

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