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欠掺杂Bi(2)Sr(2)CaCu(2)O(8+δ)晶体中的涡旋涨落

Vortex fluctuations in underdoped Bi(2)Sr(2)CaCu(2)O(8+delta) crystals.

作者信息

Colson Sylvain, Konczykowski Marcin, Gaifullin Marat B, Matsuda Yuji, Gierłowski Piotr, Li Ming, Kes Peter H, Van Der Beek Cornelis J

机构信息

Laboratoire des Solides Irradiés, CNRS-UMR 7642 and CEA/DSM/DRECAM, Ecole Polytechnique, 91128 Palaiseau, France.

出版信息

Phys Rev Lett. 2003 Apr 4;90(13):137002. doi: 10.1103/PhysRevLett.90.137002. Epub 2003 Apr 3.

Abstract

Vortex thermal fluctuations in heavily underdoped Bi(2)Sr(2)CaCu(2)O(8+delta) (T(c)=69.4 K) are studied using Josephson plasma resonance. From the zero-field data, we obtain the c-axis penetration depth lambda(L,c)(0)=230+/-10 micrometer and the anisotropy ratio gamma(T). The low plasma frequency allows us to study phase correlations over the whole vortex solid state and to extract a wandering length r(w) of vortex pancakes. The temperature dependence of r(w) as well as its increase with dc magnetic field is explained by the renormalization of the vortex line tension by the fluctuations, suggesting that this softening is responsible for the dissociation of the vortices at the first order transition.

摘要

利用约瑟夫森等离子体共振研究了严重欠掺杂的Bi(2)Sr(2)CaCu(2)O(8+δ)(T(c)=69.4 K)中的涡旋热涨落。从零场数据中,我们得到了c轴穿透深度λ(L,c)(0)=230±10微米和各向异性比γ(T)。低等离子体频率使我们能够研究整个涡旋固态中的相位关联,并提取涡旋饼的游走长度r(w)。r(w)的温度依赖性及其随直流磁场的增加可以通过涨落对涡旋线张力的重整化来解释,这表明这种软化是导致一阶转变处涡旋解离的原因。

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