...
首页> 外文期刊>Physica, C. Superconductivity and its applications >Fast vortex motion and filamentary phase separation in YBCO and TlBCCO thin films
【24h】

Fast vortex motion and filamentary phase separation in YBCO and TlBCCO thin films

机译:YBCO和TlBCCO薄膜中的快速涡旋运动和丝状相分离

获取原文
获取原文并翻译 | 示例
           

摘要

We found a correlation between the temperature dependence of the normalized magnetic relaxation rate S(T) = d In J/d In t, and the filamentary phase separation in the a-b planes of high T-c thin films, i.e., the ratio of the amount of an underdoped phase to that of an optimally doped one. These phases are characterized by different temperature dependences of the critical current density J(c)(T). J(c)(T) of the underdoped component is that of the Ginzburg-Landau (CL) one [with J(c)(T) proportional to (T-c - T)(3/2)]. For the phase closer to the optimum doping, J(c)(T) is described by the Ambegaokar-Baratoff (AB) behaviour at low temperatures with a crossover to the GL one above 0.8T(c), which is indicative of the presence of the Josephson nanostructures in the a-b planes. The results revealed that when the amount of the underdoped GL-like phase increases above a certain threshold value, a peak appears in S(T) at a temperature of 20-30 K and its height gradually increases with the magnitude of the critical current flowing through this phase. (C) 2000 Elsevier Science B.V. All rights reserved. [References: 15]
机译:我们发现归一化磁弛豫率S(T)= d In J / d In t的温度依赖性与高Tc薄膜的ab平面中的丝状相分离之间的相关性,即相对于最佳掺杂相而言,掺杂不足的相。这些相的特征在于临界电流密度J(c)(T)的不同温度依赖性。欠掺杂组分的J(c)(T)是Ginzburg-Landau(CL)的[[J(c)(T)与(T-c-T)(3/2)成比例]。对于更接近最佳掺杂的相位,J(c)(T)由低温下的Ambegaokar-Baratoff(AB)行为描述,并且在0.8T(c)以上与GL的交越点表示存在。 ab平面中的约瑟夫森纳米结构。结果表明,当欠掺杂的GL样相的数量增加到某个阈值以上时,在20-30 K的温度下S(T)中出现一个峰值,并且其高度随临界电流的大小而逐渐增加通过这个阶段。 (C)2000 Elsevier Science B.V.保留所有权利。 [参考:15]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号