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Zero-Temperature d-Wave Superconducting Phase Transition

Igor F. Herbut

DOI 10.1103/PhysRevLett.85.1532 · Physical Review Letters

T1

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Abstract

The Ginzburg-Landau-Wilson theory that describes the disordered-metal– d-wave-superconductor phase transition at zero temperature is derived at weak coupling. The theory represents an interacting dissipative system of bosonic Cooper pairs in an effective random potential. I show that there exists a wide crossover regime in the theory controlled by a line of Gaussian fixed points, each of which in two dimensions is characterized by a different universal value of the dc critical conductivity. Relation to experiments on overdoped and underdoped cuprates is discussed.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
La3Ni2O7

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—Pressure not reportedunknown
Bi2Sr2CaCu2O8+δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
(Y0.8Pr0.2)Ba2Cu3O7-δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
CsV3Sb5-xSnx

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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