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首页> 外文期刊>Diffusion and Defect Data. Solid State Data, Part B. Solid State Phenomena >Upper critical field in electron-doped superconductor with nonstoichiometric disorder near antiferromagnetic-superconducting phase boundary
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Upper critical field in electron-doped superconductor with nonstoichiometric disorder near antiferromagnetic-superconducting phase boundary

机译:反铁磁超导相边界附近具有非化学计量异常的电子掺杂超导体的上临界场

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摘要

Using the resistivity method it was found that temperature dependence of the upper critical field for underdoped Nd_(1.86)Ce_(0.14)Cu〇_(4+δ) have an anomalous upward curvature of H_(c2)(T) dependence and can be consistently explained by the two-band/two-gap model of a dirty superconductor. Near antiferromagnetic-superconducting-phase boundary the critical temperature remains constant with the change of the disorder parameter and the slope of Bc2 increases with increasing of the disorder parameter. This behavior is completely different from dependencies for pure superconducting phase at optimal doping region. This difference may indicate the change of the type of the paring: from the predominance of the anisotropic s-wave component (may be due to unstable competition between antiferromagnetic (AF) and superconducting (SC) regions) in underdoped (x=0.14) region to the prevalence of d-wave part in optimal doped regions (x=0.15) because of residual spin fluctuations.
机译:使用电阻率方法发现,对于低掺杂Nd_(1.86)Ce_(0.14)Cu〇_(4 +δ)的上临界场的温度依赖性具有H_(c2)(T)依赖性的异常上曲率,并且可以是用肮脏的超导体的两带/两间隙模型来解释。在反铁磁超导相边界附近,临界温度随无序参数的变化而保持恒定,而Bc2的斜率随无序参数的增加而增加。这种行为与在最佳掺杂区纯超导相的依赖性完全不同。这种差异可能表明配对的类型发生了变化:从各向异性s波分量的优势(可能是由于反铁磁(AF)和超导(SC)区之间的不稳定竞争)在掺杂不足(x = 0.14)的区域由于剩余自旋波动,在最佳掺杂区域(x = 0.15)中d波部分的流行率降低了。

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