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Fermion-Parity Anomaly of the Critical Supercurrent in the Quantum Spin-Hall Effect

机译:量子自旋霍尔效应中临界超电流的费米奇校验异常

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The helical edge state of a quantum spin-Hall insulator can carry a supercurrent in equilibrium between two superconducting electrodes (separation L, coherence length ζ). We calculate the maximum (critical) current I_c that can flow without dissipation along a single edge, going beyond the short-junction restriction L ? ζ of earlier work, and find a dependence on the fermion parity of the ground state when L becomes larger than ζ. Fermion-parity conservation doubles the critical current in the low-temperature, long-junction limit, while for a short junction I_c is the same with or without parity constraints. This provides a phase-insensitive, dc signature of the 4π-periodic Josephson effect.
机译:量子自旋霍尔绝缘子的螺旋边缘状态可以在两个超导电极之间保持平衡状态(间隔L,相干长度ζ)中携带超电流。我们计算出的最大(临界)电流I_c可以沿着单个边沿流过而不会耗散,超出了短接点限制L?。早期的ζ,发现当L大于ζ时,它依赖于基态的费米子奇偶性。费米子奇偶性守恒在低温长接点极限中使临界电流增加了一倍,而对于短结,I_c在有或没有奇偶性约束的情况下都相同。这提供了4π周期约瑟夫森效应的相位不敏感的dc签名。

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