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    • 8. 发明授权
    • Method for manufacturing high-temperature superconducting conductors
    • 制造高温超导导体的方法
    • US08268386B2
    • 2012-09-18
    • US11324511
    • 2006-01-03
    • Venkat SelvamanickamHee-Gyoun Lee
    • Venkat SelvamanickamHee-Gyoun Lee
    • B05D5/12H01L39/24
    • C23C16/45565C23C16/408C23C16/455C23C16/45517C23C16/45591C23C16/545H01L39/2441Y10T29/49014
    • A method for manufacturing a high-temperature superconducting conductor includes providing an elongate substrate to a reactor, the reactor having a longitudinal flow distributor. The longitudinal flow distributor has an entrance, a plurality of exits, and an interior distribution member provided between the entrance and the plurality of exits. The method further includes heating at least a portion of the substrate to a temperature sufficient to facilitate the formation of one of a superconducting material and a predecessor to a superconducting material. Further, the method includes flowing at least one precursor into the longitudinal flow distributor, through the entrance thereof, past an internal distribution member, and out through a plurality of exits, thereby longitudinally distributing the at least one precursor to form the superconducting material or predecessor thereof on the substrate.
    • 一种用于制造高温超导体导体的方法包括向反应器提供细长衬底,所述反应器具有纵向流动分配器。 纵向流动分配器具有入口,多个出口以及设置在入口和多个出口之间的内部分配构件。 该方法还包括将基底的至少一部分加热到足以有助于形成超导材料和超导材料的前身之一的温度。 此外,该方法包括将至少一种前体流经纵向流动分配器,通过其入口流过内部分配构件,并通过多个出口流出,从而纵向分配至少一种前体以形成超导材料或前身 在基板上。
    • 10. 发明授权
    • Rare-earth-Ba-Cu-O superconductors and methods of making same
    • 稀土 - Ba-Cu-O超导体及其制造方法
    • US07286032B2
    • 2007-10-23
    • US10616719
    • 2003-07-10
    • Hee-Gyoun LeeYijie LiVenkat Selvamanickam
    • Hee-Gyoun LeeYijie LiVenkat Selvamanickam
    • H01F6/00
    • H01L39/143H01L39/2461
    • Rare-earth-Ba-Cu-O superconductors having improved critical current density are described, as are methods of making same. These superconductors comprise a drop in Jc of less than a factor of about 7 at a temperature of between about 30K to about 77K, and at a magnetic field of about 1 Tesla, when the magnetic field is applied normal to the surface of the superconductor, as compared to a Jc in the presence of no magnetic field. These superconductors, when a magnetic field is applied perpendicular to the HTS surface have a peak Jc that is about 50-90%, and when a magnetic field is applied in any orientation with respect to the HTS surface have a Jc value that is at least about 50%, of the peak Jc that exists when the magnetic field is applied parallel to the surface of the superconductor.
    • 描述了具有改善的临界电流密度的稀土-BA-Cu-O超导体,以及制备它们的方法。 当施加磁场时,这些超导体在约30K至约77K之间的温度和约1特斯拉的磁场下包含小于约7的系数的小于等于7的下降 与没有磁场的场合相比,与超导体的表面垂直。 当垂直于HTS表面施加磁场时,这些超导体具有大约50-90%的峰值J,并且当相对于HTS表面以任何取向施加磁场时 具有与平行于超导体的表面施加磁场时存在的峰值Jc的至少约50%的J C值。