Abstract

Non-Fermi liquids (NFLs) are a class of strongly interacting gapless fermionic systems without long-lived quasiparticle excitations. An important group of NFL models feature itinerant fermions coupled to soft bosonic fluctuations near a quantum-critical point and are widely believed to capture the essential physics of many unconventional superconductors. However, numerically, the direct observation of a canonical NFL behavior in such systems, characterized by a power-law form in the Green's function, has been elusive. Here, we consider a Sachdev-Ye-Kitaev (SYK)-like model with random Yukawa interaction between critical bosons and fermions (dubbed the Yukawa-SYK model). We show that it is immune from the minus-sign problem and hence can be solved exactly via large-scale quantum Monte Carlo simulation beyond the large-N limit accessible to analytical approaches. Our simulation demonstrates that the Yukawa-SYK model features “self-tuned quantum criticality”; namely, the system is critical independent of the bosonic bare mass. We put these results to the test at finite N, and our unbiased numerics reveal clear evidence of these exotic quantum-critical NFL properties—the power-law behavior in the Green's function of fermions and bosons—which propels the theoretical understanding of critical Planckian metals and unconventional superconductors.2 MoreReceived 30 September 2020Accepted 24 December 2020DOI:https://doi.org/10.1103/PhysRevResearch.3.013250Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.Published by the American Physical SocietyPhysics Subject Headings (PhySH)Physical SystemsStrongly correlated systemsTechniquesNon-Fermi-liquid theoryQuantum Monte CarloSachdev-Ye-Kitaev modelCondensed Matter, Materials & Applied Physics

Highlights

  • The non-Fermi liquid (NFL) is a state of gapless fermionic matter that does not have long-lived quasiparticles due to its strongly interacting nature [1,2]

  • We put these results to the test at finite N, and our unbiased numerics reveal clear evidence of these exotic quantum-critical NFL properties—the power-law behavior in the Green’s function of fermions and bosons—which propels the theoretical understanding of critical Planckian metals and unconventional superconductors

  • Recently from studies of the Sachdev-YeKitaev (SYK) models [10,11,12,13], it has been realized that NFLs host a hidden connection between strange metals [14] and states of holographic quantum matter that saturate the upper bound for quantum chaos, opening an entirely new avenue in understanding the behavior of NFLs [15]

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Summary

INTRODUCTION

The non-Fermi liquid (NFL) is a state of gapless fermionic matter that does not have long-lived quasiparticles due to its strongly interacting nature [1,2]. For the fermionic SYK model, there is strong numerical and analytical evidence that a glass phase is absent and the NFL state persists down to T = 0 [44,45,46] For this reason the validity of the large-N analytical result of the Yukawa-SYK model needs to be carefully investigated, especially since the model involves both fermions and bosons. To this end, unbiased numeric calculations, similar in spirit to the aforementioned critical bosons Yukawa coupled to Fermi surface systems [23,24,25,26,27,29,30,31,33,47], are highly desirable. We numerically show that the bosonic Green’s function exhibits glassy behavior

THE MODEL
NFL Green’s functions
DISCUSSION
Bosonic part
Fermion determinant
Free from sign problem
Update and measurement
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