中国物理B ›› 2001, Vol. 10 ›› Issue (9): 853-856.doi: 10.1088/1009-1963/10/9/316

• • 上一篇    下一篇

CRYSTAL STRUCTURE AND MAGNETIC PROPERTIES OF La1.2Sr1.8-xCaxMn2O7

何伦华, 张泮霖, 严启伟   

  1. State Key Laboratory of Magnetism, Institute of Physics and Centre for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, China
  • 收稿日期:2001-04-23 修回日期:2001-05-09 出版日期:2001-09-15 发布日期:2005-06-12

CRYSTAL STRUCTURE AND MAGNETIC PROPERTIES OF La1.2Sr1.8-xCaxMn2O7

He Lun-hua (何伦华), Zhang Pan-lin (张泮霖), Yan Qi-wei (严启伟)   

  1. State Key Laboratory of Magnetism, Institute of Physics and Centre for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, China
  • Received:2001-04-23 Revised:2001-05-09 Online:2001-09-15 Published:2005-06-12

摘要: The effect of divalent cation substitution on the structure and magnetic properties of La1.2Sr1.8-xCaxMn2O7 (x = 0-0.900) is investigated in this paper. Partly replacing divalent cation Sr2+ by Ca2+ ions results in the weakening and then disappearance of long-range ferromagnetic ordering, and the formation of spin canting and low-temperature spin-glass. Based on structural analysis by Rietveld profile fitting, we suggest that this variation of magnetic property be related to a Jahn-Teller-type attice distortion of MnO6 octahedra due to the introduction of the smaller sized Ca2+ ions.

Abstract: The effect of divalent cation substitution on the structure and magnetic properties of La1.2Sr1.8-xCaxMn2O7 (x = 0-0.900) is investigated in this paper. Partly replacing divalent cation Sr2+ by Ca2+ ions results in the weakening and then disappearance of long-range ferromagnetic ordering, and the formation of spin canting and low-temperature spin-glass. Based on structural analysis by Rietveld profile fitting, we suggest that this variation of magnetic property be related to a Jahn-Teller-type attice distortion of MnO6 octahedra due to the introduction of the smaller sized Ca2+ ions.

Key words: structure, magnetic property, Jahn-Teller distortion

中图分类号:  (Inorganic compounds)

  • 61.66.Fn
75.30.Et (Exchange and superexchange interactions) 75.50.Cc (Other ferromagnetic metals and alloys)