Harris disorder localizes bosonic modes in quantum-critical metals, inducing compact superconducting puddles at high T and extended pairing with power-law distributed scales at low T, unlike stretched-exponential tails in disordered BCS superconductors.
Quantum Critical Eliash- berg Theory
4 Pith papers cite this work. Polarity classification is still indexing.
4
Pith papers citing it
citation-role summary
background 3
citation-polarity summary
verdicts
UNVERDICTED 4roles
background 2polarities
background 2representative citing papers
The 2D Yukawa-SYK model supplies a microscopic theory of quantum-critical incoherent metals featuring a non-Boltzmann resistivity-quasiparticle lifetime relation plus violations of the Mott-Ioffe-Regel and Kovtun-Son-Starinets bounds.
Non-Fermi liquids from critical fluctuations are grouped into seven superuniversality classes by the topology of projective fixed-point bundles, which fix universal pairing strengths and set lower bounds on superconducting transition temperatures and symmetries.
Soft loop-current fluctuations involving vanadium and antimony orbitals in kagome metals mediate chiral d+id and disorder-robust s± pairing channels, with a pressure-driven Lifshitz transition selecting between them.
citing papers explorer
-
Influence of Harris disorder on quantum-critical superconductivity
Harris disorder localizes bosonic modes in quantum-critical metals, inducing compact superconducting puddles at high T and extended pairing with power-law distributed scales at low T, unlike stretched-exponential tails in disordered BCS superconductors.
-
Universal Theory of Incoherent Metals
The 2D Yukawa-SYK model supplies a microscopic theory of quantum-critical incoherent metals featuring a non-Boltzmann resistivity-quasiparticle lifetime relation plus violations of the Mott-Ioffe-Regel and Kovtun-Son-Starinets bounds.
-
Classification of non-Fermi liquids and universal superconducting fluctuations
Non-Fermi liquids from critical fluctuations are grouped into seven superuniversality classes by the topology of projective fixed-point bundles, which fix universal pairing strengths and set lower bounds on superconducting transition temperatures and symmetries.
-
Superconductivity in kagome metals due to soft loop-current fluctuations
Soft loop-current fluctuations involving vanadium and antimony orbitals in kagome metals mediate chiral d+id and disorder-robust s± pairing channels, with a pressure-driven Lifshitz transition selecting between them.