Theory of a Strange Metal in a Quantum Superconductor to Metal Transition

Fuente: arXiv
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Main Authors: Kim, Jaewon, Berg, Erez, Altman, Ehud
Format: Preprint
Published: 2024
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author Kim, Jaewon
Berg, Erez
Altman, Ehud
author_facet Kim, Jaewon
Berg, Erez
Altman, Ehud
contents Recent experiments with nanopatterned thin films revealed an unusual quantum superconductor to metal phase transition (QSMT) with a linear in temperature resistivity. In contrast, most known examples of such transitions and standard theoretical considerations predict a temperature-independent sheet resistance of order $R_Q = \frac{\hbar}{e^2}$. We propose an effective theory of a disordered superconductor which features a QSMT with robust $T$ linear resistivity at the critical point. The crucial ingredient in our model is spatial disorder in the pairing interaction. Such random pairing mirrors the emergent phase disorder seen in a recent mean field study of a microscopic $d$-wave superconductor subject to potential disorder. We also make the prediction that in such systems the diamagnetic susceptibility diverges as $\log\fracΛ{T}$, which starkly differs from the power law divergence in standard XY transitions.
format Preprint
id arxiv_https___arxiv_org_abs_2401_17353
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Theory of a Strange Metal in a Quantum Superconductor to Metal Transition
Kim, Jaewon
Berg, Erez
Altman, Ehud
Strongly Correlated Electrons
Recent experiments with nanopatterned thin films revealed an unusual quantum superconductor to metal phase transition (QSMT) with a linear in temperature resistivity. In contrast, most known examples of such transitions and standard theoretical considerations predict a temperature-independent sheet resistance of order $R_Q = \frac{\hbar}{e^2}$. We propose an effective theory of a disordered superconductor which features a QSMT with robust $T$ linear resistivity at the critical point. The crucial ingredient in our model is spatial disorder in the pairing interaction. Such random pairing mirrors the emergent phase disorder seen in a recent mean field study of a microscopic $d$-wave superconductor subject to potential disorder. We also make the prediction that in such systems the diamagnetic susceptibility diverges as $\log\fracΛ{T}$, which starkly differs from the power law divergence in standard XY transitions.
title Theory of a Strange Metal in a Quantum Superconductor to Metal Transition
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2401.17353