English

Non-fermi liquid as passive scalar fluid

Mesoscale and Nanoscale Physics 2007-05-23 v2 Soft Condensed Matter

Abstract

I suggest that electron localization by random flux and passive transport in quenched velocity fields in two dimensions be studied as perturbations of the simple operator K=A{\cal K}={\bf A} \cdot \nabla, with incompressible velocity field/vector potential A=×ϕ=(y,x)ϕ{\bf A}=\nabla \times \phi=(-\partial_y,\partial_x)\phi. This operator has an infinitely degenerate subspace of zero energy eigenstates, arising from incompressibility, that are {\it extended} for generic ϕ(x)\phi({\bf x}) and are expected to remain so under perturbation. I propose that an anomaly accounts qualitatively for properties of the spectrum and eigenstates of K{\cal K} and its perturbations.

Cite

@article{arxiv.cond-mat/9906398,
  title  = {Non-fermi liquid as passive scalar fluid},
  author = {Jonathan Miller},
  journal= {arXiv preprint arXiv:cond-mat/9906398},
  year   = {2007}
}

Comments

Revised presentation; typographical errors corrected; no change in content

R2 v1 2026-07-22T12:12:53.518Z