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铜钡钙铜氧化物的超导态特性

Superconducting State Properties of CuBaCaCuO.

作者信息

Lynnyk Artem, Puzniak Roman, Shi Luchuan, Zhao Jianfa, Jin Changqing

机构信息

Institute of Physics, Polish Academy of Sciences, Aleja Lotników 32/46, PL-02668 Warsaw, Poland.

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.

出版信息

Materials (Basel). 2023 Jul 20;16(14):5111. doi: 10.3390/ma16145111.

DOI:10.3390/ma16145111
PMID:37512384
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10383888/
Abstract

The superconducting state properties of the CuBaCaCuO (Cu-1234) system, with a transition temperature as high as 117.5 K, were investigated. The ac magnetic susceptibility measurements confirmed a very sharp transition to the superconducting state. The upper critical field, , as high as 91 T, and the irreversibility field, , as high as 21 T at 77 K, were determined using dc SQUID magnetization measurements. The intragrain critical current density, , estimated from a magnetic hysteresis loop, is as high as 5 × 10 A/m in a self-generated magnetic field at 77 K. However, the intergrain critical current density in the studied material is smaller by four orders of magnitude due to very weak intergrain connections.

摘要

研究了转变温度高达117.5K的CuBaCaCuO(Cu-1234)体系的超导态特性。交流磁化率测量证实了向超导态的非常尖锐的转变。使用直流超导量子干涉器件(SQUID)磁化测量确定了高达91T的上临界场以及在77K时高达21T的不可逆场。根据磁滞回线估计,在77K的自生磁场中,晶粒内临界电流密度高达5×10 A/m。然而,由于晶粒间连接非常弱,所研究材料中的晶粒间临界电流密度小四个数量级。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/d8a19c6964e8/materials-16-05111-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/99c1e4d03c42/materials-16-05111-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/f4dc2743a5c5/materials-16-05111-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/71d3546a9402/materials-16-05111-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/5b152a73cd63/materials-16-05111-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/0cd7ca9d3246/materials-16-05111-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/ab0b239d851f/materials-16-05111-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/0af44ef981a2/materials-16-05111-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/c378ce096fa2/materials-16-05111-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/d8a19c6964e8/materials-16-05111-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/99c1e4d03c42/materials-16-05111-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/f4dc2743a5c5/materials-16-05111-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/71d3546a9402/materials-16-05111-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/5b152a73cd63/materials-16-05111-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/0cd7ca9d3246/materials-16-05111-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/ab0b239d851f/materials-16-05111-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/0af44ef981a2/materials-16-05111-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/c378ce096fa2/materials-16-05111-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e84c/10383888/d8a19c6964e8/materials-16-05111-g009.jpg

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