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Critical current anisotropy in conventional and artificial pinningcenter round wire Nb-Ti superconductors

机译:常规和人工钉扎中心圆线Nb-Ti超导体的临界电流各向异性

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Critical current density anisotropy was detected in conventional and artificial pinning center (APC) Nb-Ti round wires by means of a relevant increase of the magnetization M as the wire aspect ratio Aw (length L/filament diameter df) was increased. However, contrary to what is observed in APC wires, the critical current density J|| calculated from the SQUID measured saturated-magnetization in conventional wires using an anisotropic Bean model (BM), is significantly different from the transport critical current density Jct. We suggest that the mismatch between SQUID measured J|| and Jct is due to a combination of the discontinuity of the ribbons along the wire length in conventional Nb-Ti wires and also to the low electric fields generated in SQUID measurements. The low electric fields allows the magnetization-induced currents to redistribute inside the wire due to the local inhomogeneities associated with the presence of α-Ti ribbons. In this case anisotropic BM cannot be used to extract Jc from M because it will be function of the intrinsic lengths of these ribbons
机译:在常规和人工钉扎中心(APC)的Nb-Ti圆导线中,随着导线纵横比Aw(长度L /丝直径df)的增加,磁化强度M的相应增加,可以检测到临界电流密度各向异性。但是,与在APC导线中观察到的相反,临界电流密度J ||使用各向异性Bean模型(BM)根据常规导线中SQUID测得的饱和磁化强度计算出的电流与传输临界电流密度Jct明显不同。我们建议SQUID测量的J ||之间不匹配。 Jct是由于常规Nb-Ti导线中带沿导线长度的不连续性以及SQUID测量中产生的低电场的综合作用。由于与α-Ti碳带的存在有关的局部不均匀性,低电场使磁化感应电流在导线内重新分布。在这种情况下,各向异性BM不能用于从M中提取Jc,因为它将是这些带的本征长度的函数

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