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Generic nodeless Larkin-Ovchinnikov states due to singlet-triplet mixing in organic superconductors

Z. Zheng, D. F. Agterberg

DOI 10.1103/PhysRevB.82.024506 · Physical Review B

T1

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Abstract

Larkin-Ovchinnikov (LO) states typically have a singlet gap that vanishes along real-space lines. These real-space nodes lead to Andreev midgap states which can serve as a signature of LO pairing. We show that at these nodes, an odd-parity, spin-triplet component is always induced, leading to a nodeless LO phase. We find the two-dimensional weak coupling, clean limit s wave phase diagram when this spin-triplet part is included. The triplet component is large and increases the stability of the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) phase. We also show that the spin-triplet contribution pushes the midgap states away from zero energy. Finally, we show how our results can be explained phenomenologically though Lifshitz invariants. These invariants provide a simple approach to understand the role of unconventional pairing states, spin-orbit coupling, and inhomogeneous mixed singlet-triplet states that are not due to an FFLO instability. We discuss our results in the context of organic superconductors.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
κ-(BEDT-TTF)2Cu(NCS)2

Archive — visibility unverified

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

—Pressure not reportedunknown
λ-(BETS)2GaCl4

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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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