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Upper limit of metastability of the vortex-free state of a two-dimensional superconductor in a nonuniform magnetic field

机译:二维超导体在非均匀磁场中无涡态的亚稳态上限

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We calculate the magnetic field above which vortices necessarily appear in a two-dimensional superconducting film in a nonuniform magnetic field applied near its center, as in two-coil measurements of superfluid density. Experiments suggest that free vortices appear when the Meissner screening current density is large enough that the free-energy barrier for separating tightly-bound vortex-antivortex (V-aV) pairs into free vortices is comparable to k_BT, not at the much lower thermodynamic critical field. Specifically, we calculate the applied magnetic field above which there exists no metastable state without vortices. There is a simple analogy with the appearance of phase-slip centers in a one-dimensional superconducting wire.
机译:我们计算出一个磁场,在该磁场之上,涡旋必定会在二维超导薄膜中的中心附近施加一个不均匀的磁场,就像在超流体密度的两个线圈测量中一样。实验表明,当迈斯纳筛选电流密度足够大以至于将紧密结合的涡旋-反涡旋(V-aV)对分离成自由涡旋的自由能垒与k_BT相当时,就会出现自由旋涡,而不是在低得多的热力学临界值下发生领域。具体来说,我们计算施加的磁场,在该磁场之上没有涡旋就没有亚稳态。一个简单的类比就是一维超导线中相移中心的出现。

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