论文标题

非中心超导体中Chandrasekhar-Kendall州的同类

Counterpart of the Chandrasekhar-Kendall state in noncentrosymmetric superconductors

论文作者

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

论文摘要

我们证明,反转对称性的超导体支持一个自我结磁场的稳定,空间局部构型的家族。这些解决方案是我们称``toroflux''是Chandrasekhar-Kendall状态(Spheromaks)的超导对应物,它们出现在高度指挥,无力的天体物理和核融合等离子体中。在存在与$ o $ $ $点组对称性相关的奇偶校验的LIFSHITZ的情况下,超导曲线是超导模型的解决方案。这些溶液的特征在于磁场的非变化螺旋,也是磁场的环形偶极矩。我们证明,磁偶极子或铁磁包含在大部分非中心对称超导体源的有限能量toroflux溶液中。

We demonstrate that superconductors with broken inversion symmetry support a family of stable, spatially localized configurations of the self-knotted magnetic field. These solutions, that 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 non-vanishing 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.

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