Strong-coupling superconductivity near Gross-Neveu quantum criticality in Dirac systems

Fuente: arXiv
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Main Authors: Stangier, Veronika C., Sheehy, Daniel E., Schmalian, Jörg
Format: Preprint
Published: 2025
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author Stangier, Veronika C.
Sheehy, Daniel E.
Schmalian, Jörg
author_facet Stangier, Veronika C.
Sheehy, Daniel E.
Schmalian, Jörg
contents We study two-dimensional massless Dirac fermions at neutrality, coupled to bosonic modes through a Yukawa interaction. We then examine the intriguing possibility that such a system, devoid of carriers at zero temperature, might nevertheless exhibit superconductivity. Remarkably, we find that superconductivity emerges in the vicinity of Gross-Neveu quantum criticality, provided the fermions cease to behave as well-defined quasiparticles, that is, once their anomalous dimension in the normal state becomes sufficiently large. In other words, well-defined fermions do not superconduct, whereas ill-defined ones do. We analyze four symmetry-distinct bosonic modes, each capable of driving normal-state criticality and, in three of the four cases, giving rise to a distinct superconducting phase. While phase fluctuations are strong in this regime, we argue that they do not destroy the superconducting state. We further characterize the resulting pairing states for a concrete Dirac model of spin-orbit coupled systems with orbitals of different parity. Our results are obtained using the SYK-inspired framework for Dirac systems introduced by Kim et al.[1], which provides a controlled approach to the strongly coupled regime of Dirac fluids near Gross-Neveu criticality.
format Preprint
id arxiv_https___arxiv_org_abs_2509_25318
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Strong-coupling superconductivity near Gross-Neveu quantum criticality in Dirac systems
Stangier, Veronika C.
Sheehy, Daniel E.
Schmalian, Jörg
Strongly Correlated Electrons
Superconductivity
High Energy Physics - Theory
We study two-dimensional massless Dirac fermions at neutrality, coupled to bosonic modes through a Yukawa interaction. We then examine the intriguing possibility that such a system, devoid of carriers at zero temperature, might nevertheless exhibit superconductivity. Remarkably, we find that superconductivity emerges in the vicinity of Gross-Neveu quantum criticality, provided the fermions cease to behave as well-defined quasiparticles, that is, once their anomalous dimension in the normal state becomes sufficiently large. In other words, well-defined fermions do not superconduct, whereas ill-defined ones do. We analyze four symmetry-distinct bosonic modes, each capable of driving normal-state criticality and, in three of the four cases, giving rise to a distinct superconducting phase. While phase fluctuations are strong in this regime, we argue that they do not destroy the superconducting state. We further characterize the resulting pairing states for a concrete Dirac model of spin-orbit coupled systems with orbitals of different parity. Our results are obtained using the SYK-inspired framework for Dirac systems introduced by Kim et al.[1], which provides a controlled approach to the strongly coupled regime of Dirac fluids near Gross-Neveu criticality.
title Strong-coupling superconductivity near Gross-Neveu quantum criticality in Dirac systems
topic Strongly Correlated Electrons
Superconductivity
High Energy Physics - Theory
url https://arxiv.org/abs/2509.25318