Somak Basistha, Soumyajit Mandal, John Jesudasan, Vivas Bagwe and Pratap Raychaudhuri
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引用次数: 0
摘要
我们研究了两种 II 型超导薄膜涡旋态的低频电动力学,即中强引脚氮化铌(NbN)薄膜和极弱引脚非晶钼锗(a-MoGe)薄膜。我们采用双线圈互感技术来提取复合穿透深度(.)。我们采用 Coffey 和 Clem 开发的模型(CC 模型)来提取不同的涡流晶格(VL)参数,如恢复引脚力常数(拉布什参数)、VL 阻力系数和引脚势垒。我们发现,只有当我们认为旋涡上的粘性阻力比根据巴丁-斯蒂芬模型估计的粘性阻力大几个数量级时,才有可能对响应的感应和耗散部分进行一致的描述。
Low-frequency electrodynamics in the mixed state of superconducting NbN and a-MoGe films using two-coil mutual inductance technique
We investigate the low-frequency electrodynamics in the vortex state of two type-II superconducting films, namely, a moderate-to-strongly pinned Niobium Nitride (NbN) and a very weakly pinned amorphous Molybdenum Germanium (a-MoGe) film. We employ a two-coil mutual inductance technique to extract the complex penetration depth, . The sample response is studied through the temperature variation of in the mixed state, where we employ a model developed by Coffey and Clem (the CC model) to extract different vortex lattice (VL) parameters, such as the restoring pinning force constant (Labusch parameter), VL drag coefficient and pinning potential barrier. We observe that a consistent description of the inductive and dissipative part of the response is only possible when we take the viscous drag on the vortices to be several orders of magnitude larger than the viscous drag estimated from the Bardeen–Stephen model.