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Magnetoresistance Hysteresis Evolution in the Granular Y-Ba-Cu-O High-Temperature Superconductor in a Wide Temperature Range

机译:颗粒Y-Ba-Cu-O高温超导体中的磁阻滞后进化在宽温度范围内

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The temperature evolution of the magnetoresistance hysteresis in the granular YBa2Cu3O7-delta high-temperature (T-C approximate to 92K) superconductor has been investigated. The measurements have been performed in the high-temperature region (78-90K) and at the liquid helium temperature (4.2K). The results obtained have been analyzed using the developed model of the behavior of transport properties of a granular high-temperature superconductor in an external magnetic field. Within the discussed model, the dissipation of the grain boundary subsystem is determined by the intergrain spacing-averaged effective field B-eff, which is a superposition of external field H and the field induced by the magnetic moments of superconducting grains. Such a consideration yields the expression B-eff(H)=H-4 pi M(H) alpha for the effective field in the intergrain medium, where M(H) is the experimental hysteretic dependence of magnetization and alpha is the parameter of magnetic flux crowding in the intergrain medium. Here, the magnetoresistance is assumed to be proportional to the absolute value of the effective field: R(H) similar to |B-eff(H)|. Analysis of the experimental R(H) and M(H) dependences obtained under the same conditions for the investigated high-temperature superconductor sample showed that in the high-temperature region this parameter is alpha approximate to 25. At the low temperature (4.2K), we may state that the degree of flux crowding increases and the estimated alpha value is similar to 50. The estimates made are indicative of the strong effect of flux compression in the intergrain medium on the magnetotransport properties of the investigated granular high-temperature superconductor system. Possible reasons for a discrepancy between the developed model concepts and experimentally observed low-temperature R(H) hysteresis are analyzed.
机译:研究了粒状YBA2Cu3O7-δ高温(T-C近似至92K)超导体中磁阻滞后的温度演变。已经在高温区域(78-90K)和液氦温度(4.2K)中进行了测量。已经使用外部磁场中的颗粒高温超导体的运输性能的行为的开发模型进行了分析所获得的结果。在讨论的模型中,晶粒边界子系统的耗散由晶体间隔平均有效场B-EFF确定,这是外部场H的叠加和由超导颗粒的磁矩引起的磁场。这种考虑产生的表达B-EFF(H)=​​ H-4 PI m(H)α用于晶体介质中的有效场,其中M(H)是磁化的实验滞后依赖性,并且α是磁性的参​​数助焊剂在晶体介质中拥挤。这里,假设磁阻与有效场的绝对值成比例:R(H)类似于| B-EFF(H)|。在相同条件下获得的实验R(H)和M(H)依赖性的分析显示,在高温区域中,该参数是α近似为25.在低温下(4.2K ),我们可能说明助焊剂拥挤程度增加,并且估计的α值类似于50.所做的估计表明在研究颗粒高温超导体的磁传输性质上的磁化介质中的磁通压介质中的助焊剂压缩的强劲效果系统。分析了开发的模型概念和实验观察到的低温R(h)滞后之间差异的可能原因。

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