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Spin-symmetric solution of an interacting quantum dot attached to superconducting leads: Andreev states and the $0-\pi$ transition

机译:附着量子点的自旋对称解   超导线索:andreev声明和$ 0- \ pi $过渡

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摘要

Behavior of Andreev gap states in a quantum dot with Coulomb repulsionsymmetrically attached to superconducting leads is studied via the perturbationexpansion in the interaction strength. We find the exact asymptotic form of thespin-symmetric solution for the Andreev states continuously approaching theFermi level. We thereby derive a critical interaction at which the Andreevstates at zero temperature merge at the Fermi energy, being the upper bound forthe $0-\pi$ transition. We show that the spin-symmetric solution becomesdegenerate beyond this interaction, in the $\pi$ phase, and the Andreev statesdo not split unless the degeneracy is lifted. We further demonstrate that thedegeneracy of the spin-symmetric state extends also into the $0$ phase in whichthe solutions with zero and non-zero frequencies of the Andreev states maycoexist.
机译:通过相互作用强度的扰动展开,研究了库仑斥力对称地附着在超导引线上的量子点中安德列夫间隙态的行为。我们发现不断接近费米能级的安德列夫状态的自旋对称解的精确渐近形式。因此,我们得出了一个关键的相互作用,在零温度下,Andreevstates在费米能量处合并,这是$ 0- \ pi $跃迁的上限。我们证明,自旋对称解在$ \ pi $阶段变得退化超过此相互作用,并且除非解除退化,否则Andreev状态不会分裂。我们进一步证明,自旋对称态的简并性还扩展到了$ 0 $阶段,在该阶段可以同时存在具有零和非零频率的Andreev态的解。

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