Field penetration depth in RBa2Cu3O7-y, R=Y and Gd

H. C. Yang; B. D. Yao; H. E. Horng

doi:10.1088/0953-2048/1/3/011

Field penetration depth in RBa₂Cu₃O_7-y, R=Y and Gd

H. C. Yang^*, B. D. Yao, H. E. Horng

^*此作品的通信作者

研究成果: 雜誌貢獻 › 期刊論文 › 同行評審

4 引文斯高帕斯（Scopus）

摘要

The temperature dependence of the London penetration depth, lambda (T), has been determined by measuring the low-field magnetisation for RBa ₂Cu₃O_7-y samples, where R=Y and Gd. The lambda (0) value obtained from the magnetic measurement was about 0.6 mu m for both GdBa₂Cu₃O_7-y and YBa₂Cu ₃O_7-y. The lambda (T) was compared with the empirical law: lambda (T)= lambda (0)(1-(T/T_c)⁴)^-12/. The results are discussed.

原文	英語
文章編號	011
頁（從 - 到）	160-162
頁數	3
期刊	Superconductor Science and Technology
卷	1
發行號	3
DOIs	https://doi.org/10.1088/0953-2048/1/3/011
出版狀態	已發佈 - 1988 十二月 1

ASJC Scopus subject areas

陶瓷和複合材料
凝聚態物理學
金屬和合金
電氣與電子工程
材料化學

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abstract = "The temperature dependence of the London penetration depth, lambda (T), has been determined by measuring the low-field magnetisation for RBa 2Cu3O7-y samples, where R=Y and Gd. The lambda (0) value obtained from the magnetic measurement was about 0.6 mu m for both GdBa2Cu3O7-y and YBa2Cu 3O7-y. The lambda (T) was compared with the empirical law: lambda (T)= lambda (0)(1-(T/Tc)4)-12/. The results are discussed.",

author = "Yang, {H. C.} and Yao, {B. D.} and Horng, {H. E.}",

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AU - Yang, H. C.

AU - Yao, B. D.

AU - Horng, H. E.

PY - 1988/12/1

Y1 - 1988/12/1

N2 - The temperature dependence of the London penetration depth, lambda (T), has been determined by measuring the low-field magnetisation for RBa 2Cu3O7-y samples, where R=Y and Gd. The lambda (0) value obtained from the magnetic measurement was about 0.6 mu m for both GdBa2Cu3O7-y and YBa2Cu 3O7-y. The lambda (T) was compared with the empirical law: lambda (T)= lambda (0)(1-(T/Tc)4)-12/. The results are discussed.

AB - The temperature dependence of the London penetration depth, lambda (T), has been determined by measuring the low-field magnetisation for RBa 2Cu3O7-y samples, where R=Y and Gd. The lambda (0) value obtained from the magnetic measurement was about 0.6 mu m for both GdBa2Cu3O7-y and YBa2Cu 3O7-y. The lambda (T) was compared with the empirical law: lambda (T)= lambda (0)(1-(T/Tc)4)-12/. The results are discussed.

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Field penetration depth in RBa2Cu3O7-y, R=Y and Gd

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Field penetration depth in RBa₂Cu₃O_7-y, R=Y and Gd