Abstract

We study critical Fermi surfaces in generic dimensions arising from coupling finite-density fermions with transverse gauge fields, by applying the dimensional regularization scheme developed previously [Phys. Rev. B 92, 035141 (2015)]. We consider the cases of $U(1)$ and $U(1)\times U(1)$ transverse gauge couplings, and extract the nature of the renormalization group (RG) flow fixed points as well as the critical scalings. Our analysis allows us to treat a critical Fermi surface of a generic dimension $m$ perturbatively in an expansion parameter $\epsilon =\left (2-m \right ) /\left (m+1 \right).$ One of our key results is that although the two-loop corrections do not alter the existence of an RG flow fixed line for certain $U(1)\times U(1)$ theories, which was identified earlier for $m=1$ at one-loop order, the third-order diagrams do. However, this fixed line feature is also obtained for $m>1$, where the answer is one-loop exact due to UV/IR mixing.

Highlights

  • Metallic states that lie beyond the framework of LandauFermi liquid theory are often dubbed non-Fermi liquids

  • II we review the framework for applying a dimensional regularization scheme to access the non-Fermi liquid fixed points perturbatively, and apply it to the case of a single transverse gauge field

  • Ising-nematic quantum critical point, to the case of non-Fermi liquids arising from transverse gauge field couplings with finite-density fermions

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Summary

INTRODUCTION

Metallic states that lie beyond the framework of LandauFermi liquid theory are often dubbed non-Fermi liquids. We first consider an m-dimensional Fermi surface, which is coupled to a U (1) transverse gauge field a in d = (m + 1) space dimensions. The rotational symmetry of the bare fermion kinetic part in the (d − m)-dimensional space spanned by K components is destroyed by the coupling with the gauge boson, as the latter involves the γ0 matrix. With this in mind, we will denote the extra (unphysical) codimensions by the vector Kand the corresponding gamma matrices by.

Dimensional regularization
RG flows at one-loop order
Higher-loop corrections
Renormalization of the 2kF scattering amplitude
Thermodynamic quantities
CONCLUSION
One-loop fermion self-energy
One-loop vertex correction
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