TY - JOUR

T1 - Fermionic propagators for two-dimensional systems with singular interactions

AU - Sedrakyan, Tigran A.

AU - Chubukov, Andrey V.

PY - 2009/3/3

Y1 - 2009/3/3

N2 - We analyze the form of the fermionic propagator for two-dimensional fermions interacting with massless overdamped bosons. Examples include a nematic and Ising ferromagnetic quantum-critical points and fermions at a half-filled Landau level. Fermi-liquid behavior in these systems is broken at criticality by a singular self-energy, but the Fermi surface remains well defined. These are strong-coupling problems with no expansion parameter other than the number of fermionic species, N. The two known limits, N 1 and N=0, show qualitatively different behavior of the fermionic propagator G (k, ω). In the first limit, G (k, ω) has a pole at some k; in the other it is analytic. We analyze the crossover between the two limits. We show that the pole survives for all N, but at small N it only exists in a range O (N2) near the mass shell. At larger distances from the mass shell, the system evolves and G (k, ω) becomes regular. At N=0, the range where the pole exists collapses and G (k, ω) becomes regular everywhere.

AB - We analyze the form of the fermionic propagator for two-dimensional fermions interacting with massless overdamped bosons. Examples include a nematic and Ising ferromagnetic quantum-critical points and fermions at a half-filled Landau level. Fermi-liquid behavior in these systems is broken at criticality by a singular self-energy, but the Fermi surface remains well defined. These are strong-coupling problems with no expansion parameter other than the number of fermionic species, N. The two known limits, N 1 and N=0, show qualitatively different behavior of the fermionic propagator G (k, ω). In the first limit, G (k, ω) has a pole at some k; in the other it is analytic. We analyze the crossover between the two limits. We show that the pole survives for all N, but at small N it only exists in a range O (N2) near the mass shell. At larger distances from the mass shell, the system evolves and G (k, ω) becomes regular. At N=0, the range where the pole exists collapses and G (k, ω) becomes regular everywhere.

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U2 - 10.1103/PhysRevB.79.115129

DO - 10.1103/PhysRevB.79.115129

M3 - Article

AN - SCOPUS:65249155935

SN - 1098-0121

VL - 79

JO - Physical Review B - Condensed Matter and Materials Physics

JF - Physical Review B - Condensed Matter and Materials Physics

IS - 11

M1 - 115129

ER -