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arXiv 0803.0307cond-mat.supr-con
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NbSe_2单晶中的有序、无序及共存稳定涡旋晶格

Ordered, disordered and coexistent stable vortex lattices in NbSe_2 single crystals

G. Pasquini, D. Perez Daroca, C. Chiliotte, G. S. Lozano, V. Bekeris

摘要:

人们普遍认为第二类超导体临界电流密度的峰值效应是涡旋晶格有序-无序转变的结果。在其附近的涡格配置(VLC)的检查需要使用的实验技术,排除电流诱导VL重组。通过线性交流磁化率实验在坎贝尔制度,其中涡旋被迫振荡(谐波)周围的有效钉扎电位,我们探讨准静态稳定和亚稳态VLCs在NbSe_{2}单晶附近的PE。我们确定了三个不同的区域:对于T< T_{1}(H),稳定的VLC是最大有序的。当T> T_{2}(H)时,构型完全无序,未观察到亚稳态.在T_{1} <T< T_{2}区域,我们发现了具有中等无序度的温度依赖性稳定构型,这可能与整个PE中有序和无序晶格的共存有关。给出了有序畴和无序畴平衡比例的简单估计。

英文摘要:

It is commonly accepted that the peak effect (PE) in the critical current density of type II superconductors is a consequence of an order-disorder transition in the vortex lattice (VL). Examination of vortex lattice configurations (VLCs) in its vicinity requires the use of experimental techniques that exclude current induced VL reorganization. By means of linear ac susceptibility experiments in the Campbell regime, where vortices are forced to oscillate (harmonically) around their effective pinning potentials, we explore quasi-static stable and metastable VLCs in NbSe_{2} single crystals near the PE. We identify three different regions: for T<T_{1}(H), stable VLCs are maximally ordered. For T>T_{2}(H) configurations are fully disordered and no metastability is observed. In the T_{1}<T<T_{2} region we find temperature dependent stable configurations with intermediate degree of disorder, possibly associated to coexistence of ordered and disordered lattices throughout the PE. A simple estimation of the equilibrium proportion of ordered and disordered domains is provided.

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