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首页> 外文期刊>Journal of Superconductivity and Novel Magnetism >Surface Effects on the Dynamic Behavior of Vortices in Type II Superconducting Strips with Periodic and Conformal Pinning Arrays
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Surface Effects on the Dynamic Behavior of Vortices in Type II Superconducting Strips with Periodic and Conformal Pinning Arrays

机译:表面效应II型超导条带有周期性和保形钉扎阵的涡流动态行为

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Using molecular dynamics techniques, we simulate the vortex behavior in a type II superconducting strip in the presence of triangular and two types of conformal pinning arrays, one with a pinning gradient perpendicular to the driving force (C1) and the other parallel (C2), at zero temperature. A transport force is applied in the infinite direction of the strip, and the magnetic field is increased until the rate between the density of vortices (n (v) ) and pinning (n (p) ) reaches n (v) /n (p) = 1.5. Our results show a monotonic increase, by steps, of the vortex density with the applied magnetic field. Besides, each pinning lattice presents a different vortex penetration delay. For the triangular pinning array, different than the case of infinite films, here the system exhibits only one pronounced depinning force peak at n (v) /n (p) = 1. However, the depinning force peak is present for only one value of field, in the range of fields where n (v) /n (p) = 1 is stable. For the case of conformal pinning arrays, in analogy to what is observed in infinite films, no commensurability depinning force peaks were found. In the present case, the C1 array is more efficient at low fields, all arrays are equivalent in the intermediate fields, and the C2 array is more efficient for high fields. We also show that for the C1 array at high fields, vortices depin following the conformal arches, from the edge to the center. For the C2 array, the depinning force is higher when compared to that of C1, because this particular conformal structure prevents the formation of easy vortex flow channels.
机译:使用分子动力学技术,我们在三角形和两种类型的共形钉阵列的存在下模拟II型超导条带中的涡流行为,一个具有垂直于驱动力(C1)和另一个并联(C2)的钉扎梯度,在零温度下。在条带的无限方向上施加输送力,并且磁场增加到涡流密度之间的速率(n(v))和钉扎(n(p))达到n(v)/ n(p )= 1.5。我们的结果显示了单调,逐步增加涡流密度与所施加的磁场。此外,每个固定格子呈现出不同的涡流渗透延迟。对于三角形钉扎阵列,与无限膜的情况不同,这里系统在N(v)/ n(p)= 1处仅表现出一个明显的脱脂力峰值。然而,脱落力峰仅存在一个值字段,在n(v)/ n(p)= 1是稳定的场的范围内。对于保形钉扎阵列的情况,类似于在无限膜中观察到的内容,未发现脱脂力峰的不敏感性。在当前情况下,C1阵列在低场更有效,所有阵列在中间场中等同,并且C2阵列对于高领域更有效。我们还表明,对于高领域的C1阵列,涡流后的漩涡,从边缘到中心。对于C2阵列,与C1的C1相比,脱落力更高,因为该特定的保形结构防止了易于涡流流动通道的形成。

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