Pseudogaps: A third peak in the fermion spectral function

Details Pseudogaps: A third peak in the fermion spectral function Pseudogaps: A third peak in the fermion spectral function

1997-10-07

arxiv.org/abs/cond-mat/9710061v1

Phys.Rev.B 57, 2728 (1998)

Physics

Condensed Matter

Strongly Correlated Electrons

REVTeX, 8 pages, 2 PostScript figures

Scientific paper

10.1103/PhysRevB.57.2728

I present an exactly solvable model of a pseudogap with two zero-energy fermion modes coupled to each other by a classical source of frequency omega_0 and strength |Delta|. A suitably defined fermion propagator has an infinite number of poles at frequencies that are multiple integers of omega_0. In the adiabatic limit, omega_0 << |\Delta|, the situation is qualitatively different from the static case omega_0=0: the residue of the pole at omega=0 (a remnant of the bare fermion) vanishes linearly with omega_0, a result that could not be anticipated by perturbation theory; the multiple poles of the propagator coalesce into a continuum instead of forming two single poles at +-|Delta|, which should be interpreted as inhomogeneous broadening of the Bogoliubov quasiparticles.

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