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首页> 外文期刊>Physical Review, B. Condensed Matter >Fluctuation specific heat in multilayered superconductors: Bilayered Gaussian-Ginzburg-Landau scenario for the thermal fluctuations of Cooper pairs around T-c in YBa2Cu3O7-delta single crystals
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Fluctuation specific heat in multilayered superconductors: Bilayered Gaussian-Ginzburg-Landau scenario for the thermal fluctuations of Cooper pairs around T-c in YBa2Cu3O7-delta single crystals

机译:多层超导体中的涨落比热:YGa2Cu3O7-δ单晶中T-c周围库珀对的热涨落的双层高斯-金茨堡-朗道方案

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摘要

The effects around the superconducting transition of thermal fluctuations of Cooper pairs on the heat capacity in zero applied magnetic field (H=0) are explicitly calculated in bilayered superconductors, with two superconducting layers and tunneling couplings per layer periodicity length. The calculations are performed on the grounds of a generalization to multilayered superconductors of the Lawrence-Doniach Ginzburg-Landau functional, and assuming Gaussian fluctuations. In addition to the fluctuation heat capacity c(fl), we also obtain various useful relationships between c(fl) and other fluctuation-induced observables experimentally accessible in multilayered copper oxide superconductors. It is then shown that if the effects of the multilaminarity are taken into account, the mean-field-like Gaussian-Ginzburg-Landau approach may explain simultaneously and at a quantitative level the available experimental data, both the amplitude and the epsilon behavior, of the fluctuation specific heat, the in-plane paraconductivity Delta sigma(ab) and the fluctuation-induced diamagnetism Delta chi(ab) in YBa2Cu3O7-delta(Y-123) single crystals under zero or weak magnetic fields (H -->0), up to reduced temperatures of the order of epsilon=T-T-clT(c) similar to 10(-2). The corresponding coherence length amplitudes (at T = 0 K) are xi(ab)(0)= 1.1 nm and xi(c)(0) = 0.12 nm for the in-plane (ab) and transversal (c) directions, respectively. In contrast, the same data cannot be explained, in the same epsilon region, in terms of the 3DXY theory for full-critical fluctuations with a value of the dynamic critical exponent of z = 3/2, which corresponds to the same universality class as the superfluid-normal lambda transition of He-4 liquid, although these analyses do not exclude the applicability of such a scenario for epsilon less than or equal to 10(-2), as suggested by previous measurements of Delta sigma(ab) and Delta chi(ab) in the same Y-123 single crystals. However, another dynamic universality class, with z = 2, makes the 3DXY full-critical behavior compatible with the experimental data for 2 x 10(-2) less than or equal to epsilon less than or equal to 10(-1). [References: 54]
机译:在双层超导体中明确计算了库珀对热涨落的超导转变对零磁场(H = 0)中的热容的影响,该超导体具有两层超导层,每层周期长度具有隧道耦合。计算是基于劳伦斯-多尼亚奇·金斯堡-朗道泛函的多层超导体的一般化,并假设高斯涨落。除了波动热容c(fl),我们还获得了c(fl)与其他在多层氧化铜超导体中实验可获得的波动引起的可观测量之间的各种有用关系。然后表明,如果考虑到多层效应,类似平均场的高斯-金茨堡-兰道方法可以同时并定量地解释可用的实验数据,包括振幅和ε行为。零磁场或弱磁场(H-> 0)下YBa2Cu3O7-δ(Y-123)单晶的涨落比热,面内准导电性Delta sigma(ab)和涨落引起的反磁性Delta chi(ab) ,直到降低的epsilon = TTc lT(c)量级的温度类似于10(-2)。对于面内(ab)和横向(c)方向,相应的相干长度幅度(在T = 0 K时)分别为xi(ab)(0)= 1.1 nm和xi(c)(0)= 0.12 nm 。相反,在相同的epsilon区域中,对于3dXY理论,对于动态临界指数为z = 3/2的全临界波动,不能解释相同的数据,这对应于与He-4液体的超流体-正常Lambda跃迁,尽管这些分析并未排除这种情况适用于小于或等于10(-2)的ε的情况,如先前对Delta sigma(ab)和Delta的测量所暗示的那样在相同的Y-123单晶中可形成chi(ab)。但是,z = 2的另一个动态通用性类别使3DXY全临界行为与2 x 10(-2)小于或等于epsilon小于或等于10(-1)的实验数据兼容。 [参考:54]

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