超导HoMo 6 Se 8上临界磁场的研究

Tadesse Desta, Pooran Singh, G. Kahsay
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引用次数: 1

摘要

本文对超导材料hom6se8的上临界磁场进行了数学方面的研究。在零外加磁场条件下,hom6se8在5.6 K温度下由正常状态转变为超导状态,在0.3 ~ 0.53 K温度范围内恢复为正常但有序的磁态。本工作的主要目的是利用Ginzburg-Landau (GL)现象学方程来显示超导hom6se8的上临界磁场的温度依赖性。我们发现了GL相干长度(ξGL)和穿透深度(λGL)与温度之间的直接关系。根据GL方程和GL相干长度的计算结果,得到了超导材料hom6se8的上临界磁场(Hc2)表达式。结果被绘制成温度的函数。该图显示了上临界磁场(Hc2)与温度(T)的线性关系,我们的发现与实验观察一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Study of Upper Critical Magnetic Field of Superconducting HoMo 6 Se 8
This work focuses on the study of mathematical aspects of upper critical magnetic field of superconducting HoMo6Se8. At zero external magnetic field, HoMo6Se8 was found to undergo a transition from the normal state to the superconducting state at 5.6 K and returned to a normal but magnetically ordered state between the temperature range of 0.3 K and 0.53 K. The main objective of this work is to show the temperature dependence of the upper critical magnetic field of superconducting HoMo6Se8 by using the Ginzburg-Landau (GL) phenomenological Equation. We found the direct relationship between the GL coherence length (ξGL) and penetration depth (λGL) with temperature. From the GL Equations and the results obtained for the GL coherence length, the expression for upper critical magnetic field (Hc2) is obtained for the superconducting HoMo6Se8. The result is plotted as a function of temperature. The graph shows the linear dependence of upper critical magnetic field (Hc2) with temperature (T) and our finding is in agreement with experimental observations.
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