Reduction of hysteresis loss in itinerant-electron metamagnetic transition by partial substitution of Pr for La in La(FexSi1-x)13

S. Fujieda; A. Fujita; K. Fukamichi

doi:10.1016/j.jmmm.2006.10.960

Reduction of hysteresis loss in itinerant-electron metamagnetic transition by partial substitution of Pr for La in La(Fe_xSi_1-x)₁₃

S. Fujieda, A. Fujita, K. Fukamichi

Division of Inorganic Material Research

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

32 Citations (Scopus)

Abstract

The magnetocaloric effects (MCEs) and hysteresis loss in the itinerant-electron metamagnetic (IEM) transition process of La(Fe_0.86Si_0.14)₁₃ have been investigated by the partial substitution of Pr for La. The La_0.3Pr_0.7(Fe_0.86Si_0.14)₁₃ exhibits large MCEs in the magnetic field change from 0 to 5 T, which are almost the same as those of the higher Fe concentration of La(Fe_0.88Si_0.12)₁₃. Additionally, hysteresis loss in the IEM transition process of the former is smaller than that of the latter. Consequently, the La_1-zPr_z(Fe_xSi_1-x)₁₃ compounds are useful to realize large MCEs with smaller hysteresis loss as compared with that of La(Fe_xSi_1-x)₁₃.

Original language	English
Pages (from-to)	e1004-e1005
Journal	Journal of Magnetism and Magnetic Materials
Volume	310
Issue number	2 SUPPL. PART 3
DOIs	https://doi.org/10.1016/j.jmmm.2006.10.960
Publication status	Published - 2007 Mar 1

Keywords

Magnetic refrigeration
Magnetocaloric effect

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics

Access to Document

10.1016/j.jmmm.2006.10.960

Fingerprint Dive into the research topics of 'Reduction of hysteresis loss in itinerant-electron metamagnetic transition by partial substitution of Pr for La in La(FexSi1-x)13'. Together they form a unique fingerprint.

Cite this

@article{991f4c5591434518a6b37e38e6f13cc2,

title = "Reduction of hysteresis loss in itinerant-electron metamagnetic transition by partial substitution of Pr for La in La(FexSi1-x)13",

abstract = "The magnetocaloric effects (MCEs) and hysteresis loss in the itinerant-electron metamagnetic (IEM) transition process of La(Fe0.86Si0.14)13 have been investigated by the partial substitution of Pr for La. The La0.3Pr0.7(Fe0.86Si0.14)13 exhibits large MCEs in the magnetic field change from 0 to 5 T, which are almost the same as those of the higher Fe concentration of La(Fe0.88Si0.12)13. Additionally, hysteresis loss in the IEM transition process of the former is smaller than that of the latter. Consequently, the La1-zPrz(FexSi1-x)13 compounds are useful to realize large MCEs with smaller hysteresis loss as compared with that of La(FexSi1-x)13.",

keywords = "Magnetic refrigeration, Magnetocaloric effect",

author = "S. Fujieda and A. Fujita and K. Fukamichi",

year = "2007",

month = mar,

day = "1",

doi = "10.1016/j.jmmm.2006.10.960",

language = "English",

volume = "310",

pages = "e1004--e1005",

journal = "Journal of Magnetism and Magnetic Materials",

issn = "0304-8853",

publisher = "Elsevier",

number = "2 SUPPL. PART 3",

}

TY - JOUR

T1 - Reduction of hysteresis loss in itinerant-electron metamagnetic transition by partial substitution of Pr for La in La(FexSi1-x)13

AU - Fujieda, S.

AU - Fujita, A.

AU - Fukamichi, K.

PY - 2007/3/1

Y1 - 2007/3/1

N2 - The magnetocaloric effects (MCEs) and hysteresis loss in the itinerant-electron metamagnetic (IEM) transition process of La(Fe0.86Si0.14)13 have been investigated by the partial substitution of Pr for La. The La0.3Pr0.7(Fe0.86Si0.14)13 exhibits large MCEs in the magnetic field change from 0 to 5 T, which are almost the same as those of the higher Fe concentration of La(Fe0.88Si0.12)13. Additionally, hysteresis loss in the IEM transition process of the former is smaller than that of the latter. Consequently, the La1-zPrz(FexSi1-x)13 compounds are useful to realize large MCEs with smaller hysteresis loss as compared with that of La(FexSi1-x)13.

AB - The magnetocaloric effects (MCEs) and hysteresis loss in the itinerant-electron metamagnetic (IEM) transition process of La(Fe0.86Si0.14)13 have been investigated by the partial substitution of Pr for La. The La0.3Pr0.7(Fe0.86Si0.14)13 exhibits large MCEs in the magnetic field change from 0 to 5 T, which are almost the same as those of the higher Fe concentration of La(Fe0.88Si0.12)13. Additionally, hysteresis loss in the IEM transition process of the former is smaller than that of the latter. Consequently, the La1-zPrz(FexSi1-x)13 compounds are useful to realize large MCEs with smaller hysteresis loss as compared with that of La(FexSi1-x)13.

KW - Magnetic refrigeration

KW - Magnetocaloric effect

UR - http://www.scopus.com/inward/record.url?scp=33847616899&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=33847616899&partnerID=8YFLogxK

U2 - 10.1016/j.jmmm.2006.10.960

DO - 10.1016/j.jmmm.2006.10.960

M3 - Article

AN - SCOPUS:33847616899

VL - 310

SP - e1004-e1005

JO - Journal of Magnetism and Magnetic Materials

JF - Journal of Magnetism and Magnetic Materials

SN - 0304-8853

IS - 2 SUPPL. PART 3

ER -