首页> 外文期刊>Physica, C. Superconductivity and its applications >MUTUAL-INDUCTION MEASUREMENT OF THE AC PENETRATION DEPTH IN HTSCS - THEORY OF CALIBRATION FUNCTION FOR FLAT SAMPLES UNDER AXIAL SYMMETRY
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MUTUAL-INDUCTION MEASUREMENT OF THE AC PENETRATION DEPTH IN HTSCS - THEORY OF CALIBRATION FUNCTION FOR FLAT SAMPLES UNDER AXIAL SYMMETRY

机译:HTSCS交流穿透深度的互感测量-轴向对称下扁平样品的校正函数理论。

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A contribution to find optimum mutual-induction arrangements for investigating the linear AC response properties of the pinned vortices in the mixed state of HTSC is given. In particular, the complex calibration function (mutual-induction coefficient L(12) as a function of the complex AC penetration depth lambda) is analyzed, strictly axial symmetry and flat sample geometries provided (finite disk and its limiting case of infinite platelet) assuming the radius of at least one induction coil is smaller than the sample radius. Because the sample is positioned transverse to the AC induction B, the mutual inductance becomes, in general, strongly modified by distortions of B around the sample, which results in a strong dependence of L(12)(lambda) upon certain geometry parameters and an enhanced sensitivity to lambda for selected lambda intervals. The analysis is based upon powerful analytic approximation formulae for elementary arrangements derived in a separate paper. Also, formulae to estimate the errors from irregular (eccentric) sample shapes, from the field enhancement near the disk edges as well as from treating the finite-disk problem in the limit of an infinite platelet are given. Except for ultrathin films with thickness much smaller than lambda, arrangements with both the coils at the same sample side and with the loop radii sufficiently smaller than the disk radius are favored for measurements of small lambda with D/lambda greater than or equal to 1 (D is the sample thickness), which also includes the possibility of a lambda measurement in the bulk limit D/lambda> --> infinity [References: 45]
机译:给出了寻找最佳互感装置以研究HTSC混合状态下固定涡旋的线性AC响应特性的贡献。特别是,分析了复杂的校准函数(互感应系数L(12)作为AC穿透深度λ的函数),假设严格的轴向对称性和平坦的样品几何形状(有限盘及其无限大血小板的极限情况)假定至少一个感应线圈的半径小于样本半径。由于样品的位置垂直于交流感应B,因此互感通常会由于样品周围B的畸变而发生很大变化,这导致L(12)λ对某些几何参数和在选定的 lambda 间隔内增强了对lambda的敏感性。该分析基于在另一篇论文中得出的基本排列的强大解析近似公式。此外,给出了从不规则(偏心)样本形状,圆盘边缘附近的磁场增强以及在无限血小板范围内处理有限圆盘问题来估计误差的公式。除了厚度比“λ”小得多的超薄膜外,对于在“ D /λ”大于或等于的小λ的测量,有利于将两个线圈位于同一样本侧,且环路半径充分小于圆盘半径。等于1(D是样本厚度),还包括在堆积极限 D / lambda> ->无穷大中进行λ测量的可能性[参考:45]

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