The lower critical field of U6Fe

Katsuma Yagasaki; Karl A. Gschneidner; Lance E. DeLong

doi:10.1016/0921-4526(94)91280-7

The lower critical field of U₆Fe

Katsuma Yagasaki
, Karl A. Gschneidner
, Lance E. DeLong

Physics And Astronomy

Research output: Contribution to journal › Article › peer-review

1 Scopus citations

Abstract

The magnetization curves of U₆Fe were measured at several constant temperatures by a SQUID magnetometer. The lower critical field H_c1 was determined on the basis of Bean's model. H_c1 follows a 1-( T/ T_C)⁴ dependence and its extrapolated value at T=0 is 92 Gauss. H_c1 is three orders of magnitude smaller than H_c2.

Original language	English
Pages (from-to)	1561-1562
Number of pages	2
Journal	Physica B: Condensed Matter
Volume	194-196
Issue number	PART 2
DOIs	https://doi.org/10.1016/0921-4526(94)91280-7
State	Published - Feb 2 1994

Bibliographical note

Funding Information:
by a Grant-in-Aid tor Special Project Research from the Ministry of Education, Science and Culture of Japan, and also by Research Corporationa, nd the U. S. Departmenot f Energy, Office of Basic Energy Sciences, Division of Materials Sciences,u nder Contact No. W-7405-ENG-82.

Funding

by a Grant-in-Aid tor Special Project Research from the Ministry of Education, Science and Culture of Japan, and also by Research Corporationa, nd the U. S. Departmenot f Energy, Office of Basic Energy Sciences, Division of Materials Sciences,u nder Contact No. W-7405-ENG-82.

Funders	Funder number
Division of Materials Sciences and Engineering	W-7405-ENG-82
Michigan State University-U.S. Department of Energy (MSU-DOE) Plant Research Laboratory
Office of Basic Energy Sciences
Ministry of Education, Culture, Sports, Science and Technology

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics
Electrical and Electronic Engineering

Access to Document

10.1016/0921-4526(94)91280-7

Cite this

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title = "The lower critical field of U6Fe",

abstract = "The magnetization curves of U6Fe were measured at several constant temperatures by a SQUID magnetometer. The lower critical field Hc1 was determined on the basis of Bean's model. Hc1 follows a 1-( T/ TC)4 dependence and its extrapolated value at T=0 is 92 Gauss. Hc1 is three orders of magnitude smaller than Hc2.",

author = "Katsuma Yagasaki and Gschneidner, \{Karl A.\} and DeLong, \{Lance E.\}",

note = "Funding Information: by a Grant-in-Aid tor Special Project Research from the Ministry of Education, Science and Culture of Japan, and also by Research Corporationa, nd the U. S. Departmenot f Energy, Office of Basic Energy Sciences, Division of Materials Sciences,u nder Contact No. W-7405-ENG-82.",

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doi = "10.1016/0921-4526(94)91280-7",

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AU - Yagasaki, Katsuma

AU - Gschneidner, Karl A.

AU - DeLong, Lance E.

N1 - Funding Information: by a Grant-in-Aid tor Special Project Research from the Ministry of Education, Science and Culture of Japan, and also by Research Corporationa, nd the U. S. Departmenot f Energy, Office of Basic Energy Sciences, Division of Materials Sciences,u nder Contact No. W-7405-ENG-82.

PY - 1994/2/2

Y1 - 1994/2/2

N2 - The magnetization curves of U6Fe were measured at several constant temperatures by a SQUID magnetometer. The lower critical field Hc1 was determined on the basis of Bean's model. Hc1 follows a 1-( T/ TC)4 dependence and its extrapolated value at T=0 is 92 Gauss. Hc1 is three orders of magnitude smaller than Hc2.

AB - The magnetization curves of U6Fe were measured at several constant temperatures by a SQUID magnetometer. The lower critical field Hc1 was determined on the basis of Bean's model. Hc1 follows a 1-( T/ TC)4 dependence and its extrapolated value at T=0 is 92 Gauss. Hc1 is three orders of magnitude smaller than Hc2.

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