Abstract
We analyze quantum fluctuation effects at the onset of charge or spin density wave order in two-dimensional metals with an incommensurate nesting ($2k_F$) wave vector connecting two pairs of hot spots on the Fermi surface. We first compute the momentum and frequency dependence of the fermion self-energy near the hot spots to leading order in a perturbation expansion (one loop). Non-Fermi liquid behavior with a linear (in energy) quasi-particle decay rate and a logarithmically vanishing quasi-particle weight is obtained. The momentum dependence of the self-energy entails only finite renormalizations of the Fermi velocity and the Fermi surface curvature at the hot spots. The perturbative one-loop result is not self-consistent and casts doubt on the stability of the $2k_F$ quantum critical point. We construct a self-consistent solution of the one-loop equations with self-energy feedback, where the quantum critical point is stabilized rather than being destroyed by fluctuations, while the non-Fermi liquid behavior as found in the perturbative one-loop calculation is confirmed.
Highlights
Quantum critical fluctuations at the onset of charge or spin-density wave order in two-dimensional metals destroy Fermi-liquid behavior and lead to unconventional dependencies on temperature and other control parameters [1]
In this paper we extend the analysis of fluctuation effects at the onset of 2kF density wave order with two pairs of hot spots
We focus on the frequency dependence of the self-energy at a hot spot as described by the function H =
Summary
Quantum critical fluctuations at the onset of charge or spin-density wave order in two-dimensional metals destroy Fermi-liquid behavior and lead to unconventional dependencies on temperature and other control parameters [1]. In the former case there is no competing instability on the mean-field level, and fluctuation induced pairing may set in only as a secondary instability at a low energy scale.
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