Spin fluctuations and pseudogap in the two-dimensional half-filled Hubbard model at weak coupling

dc.creatorDupuis, N.
dc.date2001-10-08
dc.date2002-07-04
dc.date.accessioned2026-07-07T06:21:45Z
dc.date.available2026-07-07T06:21:45Z
dc.descriptionStarting from the Hubbard model in the weak-coupling limit, we derive a spin-fermion model where the collective spin excitations are described by a non-linear sigma model. This result is used to compute the fermion spectral function $A({\bf k},ω)$ in the low-temperature regime where the antiferromagnetic (AF) coherence length is exponentially large (``renormalized classical'' regime). At the Fermi level, $A({\bf k}_F,ω)$ exhibits two peaks around $\pmΔ_0$ (with $Δ_0$ the mean-field gap), which are precursors of the zero-temperature AF bands, separated by a pseudogap.
dc.description6 pages, 2 figures, revised version
dc.identifierhttps://arxiv.org/abs/cond-mat/0110138
dc.identifierhttp://arxiv.org/abs/cond-mat/0110138
dc.identifierPhys. Rev. B 65, 245118 (2002)
dc.identifierdoi:10.1103/PhysRevB.65.245118
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/95704
dc.subjectStrongly Correlated Electrons
dc.titleSpin fluctuations and pseudogap in the two-dimensional half-filled Hubbard model at weak coupling
dc.typetext

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