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Infiltration growth processing of bulk mixed REBa_2Cu_3O_7-x superconductors: Nano metal oxides and rare earth elements effects on microstructural properties

机译:大块混合REBa_2Cu_3O_7-x超导体的渗透生长过程:纳米金属氧化物和稀土元素对微结构性能的影响

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摘要

The REBa_2Cu_3O_(7-x) (REBCO/YBCO) based high-temperature superconductors are promising materials for high magneticfield and energy applications due to their effective flux pinning abilities. The superconducting properties of these materialsstrongly depend on the microstructure, which could be engineered by the fabrication methods, and incorporating variousdopants. Infiltration growth (IG) process is currently evolving and superior to the standard melt growth (MG) techniqueaddressing various inherent and unwanted problems. However, the IG technique is complex as compared to conventionalMG technique, and for high reproducibility, many parameters need to be optimized for every system. In thispaper, we present the engineering of the final microstructure with various nanometric metal oxides to the bulkYBCO/REBCO materials aiming to improve the field dependence of the superconducting properties. The effect of introducingvarious RE elements in IG processed YBCO/GdBCO bulk superconductors, and the evolution of microstructuressupported by thorough elemental analysis will be discussed. Emphasis will be given to the problems involved in thegrowth of mixed REBCO products in the IG process and to the microstructural properties at various stages of processingthe bulk samples.
机译:基于REBa_2Cu_3O_(7-x)(REBCO / YBCO)的高温超导体具有有效的磁通钉扎能力,是用于高磁场和高能量应用的有前途的材料。这些材料的超导性能很大程度上取决于其微观结构,可以通过制造方法对其进行工程设计,并结合各种掺杂剂。渗透生长(IG)工艺目前正在发展,并且优于标准的熔体生长(MG)技术\ r \ n解决了各种固有的和有害的问题。但是,与传统的\ r \ nMG技术相比,IG技术非常复杂,并且为实现高重现性,需要为每个系统优化许多参数。在本文中,我们向大量的\ r \ nYBCO / REBCO材料介绍了使用各种纳米金属氧化物的最终微观结构的工程设计,旨在改善超导性能的场依赖性。讨论了在IG处理的YBCO / GdBCO体超导体中引入各种稀土元素的效果,以及通过详尽的元素分析支持的微观结构的演变。重点将放在IG工艺中混合REBCO产品的生长问题以及在大批量样品加工的各个阶段的微观结构特性。

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  • 来源
    《Superconductivity and Particle Accelerators 2018》|2018年|110540H.1-110540H.8|共8页
  • 会议地点 1996-756X;0277-786X
  • 作者单位

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305- 8568, Japan Superconducting Materials Laboratory, Graduate School of Science and Engineering, Shibaura Institute of Technology, Tokyo, 135-8548, Japan spavankumarnaik@yahoo.in;

    Dept. of Physics, Government College, Anantapur, Andhra Pradesh, India;

    Dept. of Physics, GITAM, Hyderabad, Telangana, India;

    Superconducting Materials Laboratory, Graduate School of Science and Engineering, Shibaura Institute of Technology, Tokyo, 135-8548, Japan;

    Superconducting Materials Laboratory, Graduate School of Science and Engineering, Shibaura Institute of Technology, Tokyo, 135-8548, Japan;

    Superconducting Materials Laboratory, Graduate School of Science and Engineering, Shibaura Institute of Technology, Tokyo, 135-8548, Japan;

    Superconducting Materials Laboratory, Graduate School of Science and Engineering, Shibaura Institute of Technology, Tokyo, 135-8548, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305- 8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305- 8568, Japan;

    National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305- 8568, Japan;

    Superconducting Materials Laboratory, Graduate School of Science and Engineering, Shibaura Institute of Technology, Tokyo, 135-8548, Japan;

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