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Oxide superconductor and method for manufacturing same

專利號
US12161054B2
公開日期
2024-12-03
申請人
KABUSHIKI KAISHA TOSHIBA(JP Tokyo)
發(fā)明人
Takeshi Araki; Hirotaka Ishii
IPC分類
H10N60/85; H10N60/01
技術領域
ybco,pr,region,in,coating,film,ococh3,oxide,perovskite,μm
地域: Tokyo

摘要

An oxide superconductor of an embodiment includes an oxide superconducting layer including a first superconducting region containing barium, copper, and a first rare earth element, having a continuous perovskite structure, and extending in a first direction, a second superconducting region containing barium, copper, and a second rare earth element, having a continuous perovskite structure, and extending in the first direction, and a non-superconducting region disposed between the first and the second superconducting region, containing praseodymium, barium, copper, and a third rare earth element, a ratio of the number of atoms of the praseodymium to a sum of the number of atoms of the third rare earth element and the number of atoms of the praseodymium which is 20% or more, having a continuous perovskite structure continuous with the perovskite structure of the first superconducting region and the perovskite structure of the second superconducting region, and extending in the first direction.

說明書

FIG. 7 is a diagram illustrating a typical firing profile of the first embodiment. A mixed gas is dried up to tb1 at 100° C., but humidification is performed. A humidification start temperature may be 100° C. or higher and 400° C. or lower. It seems that the formation of the quasi-liquid layer starts from around 550° C., and the humidification is performed at a temperature lower than that so that the humidifying gas spreads inside the film and the quasi-liquid layer is uniformly formed.

FIG. 7 illustrates a typical temperature profile of firing at 800° C., but the temperature rise profile is gentle at 775° C. or higher and 800° C. or lower so that there is no temperature overshoot at tb3. However, an overshoot at 800° C. can remain at 2 to 3° C., which is not particularly a problem. An oxygen partial pressure at the highest temperature depends on the matrix phase. In the case of YBCO superconductor firing, the partial pressure is 1000 ppm at 800° C., and the optimum oxygen partial pressure is halved every time the temperature drops by 25° C. That is, the partial pressure is 500 ppm at 775° C. and 250 ppm at 750° C. In the case of the YBCO system, YBa2Cu3O6 is formed in this firing. At this point, no superconductor exists.

For example, the highest temperature of firing may be 750° C. In this case, for example, the same temperature rise rate as in FIG. 7 is performed to a temperature 25° C. lower than the highest temperature, and the temperature rise rate is reduced to raise the temperature to the highest temperature.

權利要求

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