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    • 1. 发明申请
    • Superconducting magnet, process for producing the same and its magnetizing method
    • 超导磁体,其制造方法及其磁化方法
    • US20050083058A1
    • 2005-04-21
    • US10506206
    • 2003-12-12
    • Ikuo ItohHiroaki OtsukaMitsuru Sawamura
    • Ikuo ItohHiroaki OtsukaMitsuru Sawamura
    • H01F6/00H01F7/02H01F13/00H01F41/02G01V3/00
    • H01F13/003H01F6/00H01F7/02H01F41/0253
    • A superconductive magnet comprised of a bulk member or sheet member of a type II superconductive material, wherein a distribution of the magnetic flux density component vertical to the surface directly above the surface of the bulk member or sheet member (a) has a maximum value at a center of said bulk member or sheet member and is about zero at its side edge, and (b) has at least one minimal value point between said center and side edge. A superconductor is cooled to not more than a critical temperature after applying a magnetic field Hex1 [A/m] near the magnetic field generation system in the normal conductive state, then the applied magnetic field is reduced to zero, then a magnetic field is applied until the applied magnetic field becomes −Hex2 [A/m] in the opposite direction to the trapped magnetic flux to make the trapped magnetic flux density Bin0 [T], then the applied magnetic field is again returned to zero, where Hex1>0 and Hex2>0.
    • 一种由II型超导材料的主体部件或片状部件组成的超导磁体,其中垂直于大块部件或片状部件(a)表面正上方的表面的磁通密度分量的分布在 所述主体部件或片部件的中心在其侧边缘处约为零,并且(b)在所述中心和侧边之间具有至少一个最小值点。 在正常导通状态下在磁场产生系统附近施加磁场Hex1 [A / m]后,将超导体冷却至临界温度,然后施加的磁场减小到零,然后施加磁场 直到所施加的磁场与被捕获的磁通量相反的方向变为-Hex2 [A / m],以使被捕获的磁通密度Bin0 [T],则所施加的磁场再次返回到零,其中Hex1> 0和 Hex2> 0。