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首页> 外文期刊>Modern Physics Letters, B. Condensed Matter Physics, Statistical Physics, Applied Physics >Excess conductivity in the mean field and paracoherence regimes of (La1.6Y0.4)Ba2Ca0.8Cu4.8Oz superconductors
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Excess conductivity in the mean field and paracoherence regimes of (La1.6Y0.4)Ba2Ca0.8Cu4.8Oz superconductors

机译:(La1.6Y0.4)Ba2Ca0.8Cu4.8Oz超导体的平均场和超相干态中的电导率过高

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摘要

The temperature variations of electrical resistivity have been measured on pure and 5 wt% Ag doped (La1.6Y0.4)Ba2Ca0.8Cu4.8Oz superconductors. These data were analyzed in terms of fluctuation-induced excess conductivity in the mean field regime by using the Aslamazov-Larkin (AL), Lawrence-Doniach (LD) and Maki-Thompson (MT) models. The fluctuations in the amplitude of order parameter are found to be two dimensional in nature in the mean field region. The estimated values of the average phase breaking time To (100 K) are found to be 3.9 x 10(-16) s and 4.6 x 10(-16) s for pure and Ag doped samples respectively. The resistivity data were also analyzed in terms of excess conductivity due to phase fluctuations of the order parameter in the paracoherence region. The critical exponent is found to be mostly comparable to that of the 3D XY ferromagnet in the vicinity of zero resistivity temperature and the diluted Heisenberg model at a higher temperature.
机译:已经在纯的和5 wt%的Ag掺杂(La1.6Y0.4)Ba2Ca0.8Cu4.8Oz超导体上测量了电阻率的温度变化。通过使用Aslamazov-Larkin(AL),Lawrence-Doniach(LD)和Maki-Thompson(MT)模型,在平均场条件下根据波动引起的过剩电导率分析了这些数据。发现阶跃参数幅度的波动在平均场区域中本质上是二维的。对于纯样品和掺Ag样品,平均断相时间To(100 K)的估计值分别为3.9 x 10(-16)s和4.6 x 10(-16)s。由于超相干区域中阶参数的相位波动,还根据过剩的电导率对电阻率数据进行了分析。发现在零电阻率温度和更高温度下的稀薄海森堡模型附近,该临界指数几乎与3D XY铁磁体相当。

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