paper

Dynamical susceptibility near a long-wavelength critical point with a nonconserved order parameter

arXiv:1708.05308 · doi:10.1103/PhysRevB.97.155115

Abstract

We study the dynamic response of a two-dimensional system of itinerant fermions in the vicinity of a uniform () Ising nematic quantum critical point of wave symmetry. The nematic order parameter is not a conserved quantity, and this permits a nonzero value of the fermionic polarization in the wave channel even for vanishing momentum and finite frequency: . For weak coupling between the fermions and the nematic order parameter (i.e. the coupling is small compared to the Fermi energy), we perturbatively compute over a parametrically broad range of frequencies where the fermionic self-energy is irrelevant, and use Eliashberg theory to compute in the non-Fermi liquid regime at smaller frequencies, where . We find that is a constant, plus a frequency dependent correction that goes as at high frequencies, crossing over to at lower frequencies. The scaling holds also in a non-Fermi liquid regime. The non-vanishing of gives rise to additional structure in the imaginary part of the nematic susceptibility at , in marked contrast to the behavior of the susceptibility for a conserved order parameter. This additional structure may be detected in Raman scattering experiments in the wave geometry.

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