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

机译:常规和人工钉扎中心圆线Nb-Ti超导体中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 A/sub w/ (length L/filament diameter d/sub f/) was increased. However, contrary to what is observed in APC wires, the critical current density J/sub /spl par// 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 J/sub ct/. We suggest that the mismatch between SQUID measured J/sub /spl par// and J/sub ct/ 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 /spl alpha/-Ti ribbons. In this case anisotropic BM cannot be used to extract J/sub c/ from M because it will be function of the intrinsic lengths of these ribbons.
机译:在传统和人工钉扎中心(APC)的Nb-Ti圆线中,通过磁化强度M随线宽比A / sub w /(长度L /丝直径d / sub f /)增加了。但是,与在APC导线中观察到的相反,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临界电流密度J / sub / spl par //明显不同于传输临界值电流密度J / sub ct /。我们建议,SQUID测量的J / sub / spl par //和J / sub ct /之间的不匹配是由于常规Nb-Ti导线中带沿线长度的不连续性以及低电场共同造成的在SQUID测量中生成。由于与/ spl alpha / -Ti带的存在相关的局部不均匀性,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J / sub c /,因为它将是这些色带的固有长度的函数。

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