{"title":"bcc-FeRh1-xMx体系的磁性能","authors":"S. Yuasa;Y. Otani;H. Miyajima;A. Sakuma","doi":"10.1109/TJMJ.1994.4565981","DOIUrl":null,"url":null,"abstract":"The magnetic properties of ordered bcc FeRh\n<inf>1-x</inf>\nM\n<inf>x</inf>\n alloys (M=Fe, Co, Ni, Pd, Ir and Pt) were studied, in terms of correlations among the antiferromagnetic-ferromagnetic transition temperature T\n<inf>0</inf>\n, Curie temperature, magnetization, and lattice constant. Substitution of the 3d element M for Rh diminishes the transition temperature T\n<inf>0</inf>\n, since the large magnetic moment of the M atom stabilizes the ferromagnetism. Moreover, a first-order antiferromagnetic-paramagnetic transition was observed in an FeRh\n<inf>1-x</inf>\nIr\n<inf>x</inf>\n system. The mechanism of such first-order phase transitions can be explained phenomenologically by introducing magneto-volume coupling into a model based on the SCR theory. The ground state properties of FeRh and FeRh\n<inf>1-x</inf>\nPd\n<inf>x</inf>\n are well explained by first-principle band calculations based on the linearized muffin-tin orbital method.","PeriodicalId":100647,"journal":{"name":"IEEE Translation Journal on Magnetics in Japan","volume":"9 6","pages":"202-209"},"PeriodicalIF":0.0000,"publicationDate":"1994-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1109/TJMJ.1994.4565981","citationCount":"14","resultStr":"{\"title\":\"Magnetic Properties of bcc FeRh1-xMx Systems\",\"authors\":\"S. Yuasa;Y. Otani;H. Miyajima;A. Sakuma\",\"doi\":\"10.1109/TJMJ.1994.4565981\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The magnetic properties of ordered bcc FeRh\\n<inf>1-x</inf>\\nM\\n<inf>x</inf>\\n alloys (M=Fe, Co, Ni, Pd, Ir and Pt) were studied, in terms of correlations among the antiferromagnetic-ferromagnetic transition temperature T\\n<inf>0</inf>\\n, Curie temperature, magnetization, and lattice constant. Substitution of the 3d element M for Rh diminishes the transition temperature T\\n<inf>0</inf>\\n, since the large magnetic moment of the M atom stabilizes the ferromagnetism. Moreover, a first-order antiferromagnetic-paramagnetic transition was observed in an FeRh\\n<inf>1-x</inf>\\nIr\\n<inf>x</inf>\\n system. The mechanism of such first-order phase transitions can be explained phenomenologically by introducing magneto-volume coupling into a model based on the SCR theory. The ground state properties of FeRh and FeRh\\n<inf>1-x</inf>\\nPd\\n<inf>x</inf>\\n are well explained by first-principle band calculations based on the linearized muffin-tin orbital method.\",\"PeriodicalId\":100647,\"journal\":{\"name\":\"IEEE Translation Journal on Magnetics in Japan\",\"volume\":\"9 6\",\"pages\":\"202-209\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1994-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1109/TJMJ.1994.4565981\",\"citationCount\":\"14\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Translation Journal on Magnetics in Japan\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/4565981/\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Translation Journal on Magnetics in Japan","FirstCategoryId":"1085","ListUrlMain":"https://ieeexplore.ieee.org/document/4565981/","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The magnetic properties of ordered bcc FeRh
1-x
M
x
alloys (M=Fe, Co, Ni, Pd, Ir and Pt) were studied, in terms of correlations among the antiferromagnetic-ferromagnetic transition temperature T
0
, Curie temperature, magnetization, and lattice constant. Substitution of the 3d element M for Rh diminishes the transition temperature T
0
, since the large magnetic moment of the M atom stabilizes the ferromagnetism. Moreover, a first-order antiferromagnetic-paramagnetic transition was observed in an FeRh
1-x
Ir
x
system. The mechanism of such first-order phase transitions can be explained phenomenologically by introducing magneto-volume coupling into a model based on the SCR theory. The ground state properties of FeRh and FeRh
1-x
Pd
x
are well explained by first-principle band calculations based on the linearized muffin-tin orbital method.