Abstract

We study (fermionic) spectral functions in two holographic models, the Gubser-Rocha-linear axion model and the linear axion model, where translational symmetry is broken by axion fields linear to the boundary coordinates (${\ensuremath{\psi}}_{I}=\ensuremath{\beta}{\ensuremath{\delta}}_{Ii}{x}^{i}$). Here, $\ensuremath{\beta}$ corresponds to the strength of momentum relaxation. The spectral function is computed by the fermionic Green's function of the bulk Dirac equation, where a fermion mass, $m$, and a dipole coupling, $p$, are introduced as input parameters. By classifying the shape of spectral functions, we construct complete phase diagrams in ($m$, $p$, $\ensuremath{\beta}$) space for both models. We find that two phase diagrams are similar even though their background geometries are different. This similarity might be due to temperature effect, since our analysis has been done at small but finite temperature ($T/\ensuremath{\mu}=0.1$). We also find that the effect of momentum relaxation on the (spectral function) phases of two models are similar even though the effect of momentum relaxation on the dc conductivities of two models are very different. We suspect that this is because holographic fermion does not backreact to geometry in our framework.

Highlights

  • One of the important milestones in condensed matter physics is Landau’s Fermi liquid theory because it provides us a way to understand almost all metals, semiconductors, superconductors, and superfluids

  • Studying holographic “spectral function” could be an important test for the application of gauge/gravity duality because it can be compared with measurements of angle resolved photoemission spectroscopy (ARPES) or scanning tunneling microscopy (STM)

  • As in the Gubser-Rocha-linear axion model, we investigate the spectral functions at fixed chemical potential: (T=μ; β=μ)

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Summary

INTRODUCTION

One of the important milestones in condensed matter physics is Landau’s Fermi liquid theory because it provides us a way to understand almost all metals, semiconductors, superconductors, and superfluids. In addition to non-Fermi liquid, various phases of matter are discovered in strongly correlated systems such as the strange metals and high temperature superconductors [1,2,3]. The gauge/gravity duality (or AdS/CFT correspondence, or holographic methods) have provided effective tools to study such exotic phases in strongly correlated materials [4,5,6],. Which states that the strongly correlated condensed matter physics can be mapped to the classical gravity physics. Using this method, there are many studies of fermionic response in strongly correlated system. Studying holographic “spectral function” could be an important test for the application of gauge/gravity duality because it can be compared with measurements of angle resolved photoemission spectroscopy (ARPES) or scanning tunneling microscopy (STM)

Momentum relaxation
Spectral function with momentum relaxation
Motivations of this paper
Dirac equation and Green’s function
GUBSER-ROCHA-LINEAR AXION MODEL
L2 cosh φ
Zero momentum relaxation
Finite momentum relaxation
LINEAR AXION MODEL AND COMPARISON
CONCLUSION
Embedding
Symmetrized spectral function
Single site DMFT result for Hubbard model
Two site DMFT result for Hubbard model
Full Text
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