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中国物理学会期刊

多带超导体中的自发磁场和奇频配对态

CSTR: 32037.14.aps.68.20190445

Spontaneous magnetic field and odd-frequency pairing state in multiband superconductors

CSTR: 32037.14.aps.68.20190445
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  • 基于金兹堡-朗道模型, 本文研究了双带超导体硼化镁中的奇频配对态, 并证明了带间耦合可以诱导“半-涡旋”结构以及四度旋转对称与二度旋转对称的涡旋格子相变. 零外场条件下, 带间耦合可以诱导出新物质态和奇特的自发畴结构; 具体表现为, 环绕着畴壁, 该自发磁场的极性螺旋进动, 对应着局域旋转对称自发破缺, 从而允许存在时间反演破缺束缚态. 与此同时, 磁性畴壁散射引起的自旋相反的电子的费米波矢失配则允许自旋单态与自旋三重态的共存, 而一个偶宇称的三重态必将是频域奇称的配对态. 文中给出了双带硼化镁超导体普适的相图.

     

    We investigate the interband coupling induced odd-frequency pairing state by solving the microscopic Ginzburg-Landau model for the two band superconductor magnesium diboride (MgB2). It is found that the interband coupling can induce a new domain structure and a heliacal spontaneous magnetic vortex-antivortex pair around the cyclical domain wall, which breaks down spin-rotational symmetry and supports a time-reversal violating bound state, allowing the coexistence of spin-singlet and spin-triplet state close to the spontaneous vortex core. The odd-frequency spin-triplet even parity pairing state occurs since a successive operation in the orbital parity (P) and the time-reversal (T) obeys PT = + 1(–1) for spin-singlet (spin-triplet) pairing amplitude. A general phase diagram is presented.

     

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