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Counterpart of the Chandrasekhar-Kendall state in noncentrosymmetric superconductors

Julien Garaud, Anatolii Korneev, Albert Samoilenka, Alexander Molochkov, Egor Babaev, Maxim Chernodub

DOI 10.1103/PhysRevB.108.014504 · Physical Review B

T1

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Abstract

We demonstrate that superconductors with broken inversion symmetry support a family of stable, spatially localized configurations of the self-knotted magnetic field. These solutions, which we term “toroflux,” are the superconducting counterparts of the Chandrasekhar-Kendall states (spheromaks) that appear in highly conducting, force-free astrophysical and nuclear-fusion plasmas. The superconducting torofluxes are solutions of superconducting models, in the presence of a parity-breaking Lifshitz invariant associated with the O point-group symmetry. These solutions are characterized by a nonvanishing helicity of the magnetic field, and also by a toroidal dipole moment of the magnetic field. We demonstrate that a magnetic dipole or a ferromagnetic inclusion in the bulk of a noncentrosymmetric superconductor sources finite-energy toroflux solutions.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Li2Pt3B

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

—Pressure not reportedunknown
Mo3Al2C

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—Pressure not reportedunknown
PtSbS

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—Pressure not reportedunknown

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