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Geometric effects on T-breaking in p+ip and d+id superconducting arrays

J. E. Moore, D.-H. Lee

DOI 10.1103/PhysRevB.69.104511 · Physical Review B

T1

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Abstract

Superconducting order parameters that change phase around the Fermi surface modify Josephson tunneling behavior, as in the phase-sensitive measurements that confirmed d order in the cuprates. This paper studies Josephson coupling when the individual grains break time-reversal symmetry; the specific cases considered are p±ip and d±id, which may appear in Sr2RuO4 and NaxCoO2⋅(H2O)y, respectively. T-breaking order parameters lead to frustrating phases when not all grains have the same sign of time-reversal symmetry breaking, and the effects of these frustrating phases depend sensitively on geometry for two-dimensional arrays of coupled grains. These systems can show perfect superconducting order with or without macroscopic T-breaking. The honeycomb lattice of superconducting grains has a superconducting phase with no spontaneous breaking of T but instead power-law correlations. The superconducting transition in this case is driven by binding of fractional vortices, and the zero-temperature criticality realizes a generalization of Baxter’s three-color model.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
NaxCoO2*(H2O)y

Archive — visibility unverified

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

—Pressure not reportedunknown
Sr2RuO4

Archive — visibility unverified

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

—Pressure not reportedunknown

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