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Approximate Ginzburg-Landau solution for the regular flux-line lattice. Circular cell method

机译:用于常规磁通线晶格的近似Ginzburg-Landau解。   圆形细胞法

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摘要

A variational model is proposed to describe the magnetic properties oftype-II superconductors in the entire field range between $H_{c1}$ and $H_{c2}$for any values of the Ginzburg-Landau parameter $\kappa>1/\sqrt{2}$. Thehexagonal unit cell of the triangular flux-line lattice is replaced by a circleof the same area, and the periodic solutions to the Ginzburg-Landau equationswithin this cell are approximated by rotationally symmetric solutions. TheGinzburg-Landau equations are solved by a trial function for the orderparameter. The calculated spatial distributions of the order parameter and themagnetic field are compared with the corresponding distributions obtained bynumerical solution of the Ginzburg-Landau equations. The comparison revealsgood agreement with an accuracy of a few percent for all $\kappa$ valuesexceeding $\kappa \approx 1$. The model can be extended to anisotropicsuperconductors when the vortices are directed along one of the principal axes.The reversible magnetization curve is calculated and an analytical formula forthe magnetization is proposed. At low fields, the theory reduces to the Londonapproach at $\kappa \gg 1$, provided that the exact value of $H_{c1}$ is used.At high fields, our model reproduces the main features of the well-knownAbrikosov theory. The magnetic field dependences of the reversiblemagnetization found numerically and by our variational method practicallycoincide. The model also refines the limits of some approximations which havebeen widely used. The calculated magnetization curves are in a good agreementwith experimental data on high-T$_c$ superconductors.
机译:对于Ginzburg-Landau参数$ \ kappa> 1 / \ sqrt的任何值,提出了一种变分模型来描述II型超导体在$ H_ {c1} $和$ H_ {c2} $之间的整个磁场范围内的磁性能。 {2}美元。用相同面积的圆代替三角形通量线格的六边形单元格,并通过旋转对称解近似该单元格内Ginzburg-Landau方程的周期解。格林茨堡-兰道方程通过阶数参数的试验函数求解。将计算得到的阶数参数和磁场的空间分布与通过Ginzburg-Landau方程的数值解获得的相应分布进行比较。比较结果表明,对于所有超过\ kappa \ approx 1 $的$ \ kappa $值,其精度都达到百分之几。当涡流沿主轴之一指向时,该模型可以扩展到各向异性超导体。计算可逆磁化曲线,并给出磁化的解析公式。在低场下,只要使用$ H_ {c1} $的精确值,该理论就简化为$ \ kappa \ gg 1 $的伦敦方法。在高场下,我们的模型重现了著名的Abrikosov理论的主要特征。在数值上发现的可逆磁化的磁场依赖性以及通过我们的变分方法实际上是一致的。该模型还完善了一些已被广泛使用的近似值的极限。计算的磁化曲线与高T $ _c $超导体的实验数据非常吻合。

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