Structural and magnetic properties of RSr2Fe3O9 (R = La, Y, Pr, and Gd)

被引:9
作者
Awana, VPS [1 ]
Dou, SX
Felner, I
Nowik, I
Malik, SK
Mehta, A
Singh, R
Narlikar, AV
Yelon, WB
机构
[1] Univ Wollongong, Ctr Superconduct & Elect Mat, Wollongong, NSW 2522, Australia
[2] Hebrew Univ Jerusalem, Racah Inst Phys, IL-91904 Jerusalem, Israel
[3] Tata Inst Fundamental Res, Bombay 400005, Maharashtra, India
[4] Stanford Synchrotron Radiat Lab, SLAC, Stanford, CA 94309 USA
[5] Natl Phys Lab, New Delhi 110012, India
[6] Univ Missouri, Res Reactor Facil, Columbia, MO 65211 USA
关键词
D O I
10.1063/1.367834
中图分类号
O59 [应用物理学];
学科分类号
摘要
We have investigated the RSr2Fe3O9 (R=La, Y, Pr, and Gd) materials by several experimental techniques, including x-ray and neutron diffraction, magnetic susceptibility, and Mossbauer spectroscopy measurements. All materials studied are single phase and crystallize in the hexagonal perovskite structure. Magnetic susceptibility studies reveal that, for R=La and Pr, the Fe ions order antiferromagnetically at about T-N =190 K. Short range magnetic correlations are observed up to 250 K. For R = La and Pr, Fe-57 Mossbauer studies reveal two inequivalent magnetic sextets below 190 K, with the area ratio 2:1. Above T-N, one singlet is observed with an isomer shift value typical to Fe4+ For R = Y and Gd, the magnetization curves do not lend themselves to easy determination of the magnetic transition due to an extra magnetic phase which exists up to 350 K. This phase is a result of deficiency of oxygen. The (57)Mossbauer spectra at 300 K indicate two superimposed singlet lines, and contain a small magnetic sextet. There is no indication that the R sublattice in RSr2Fe3O9 (R=Pr and Gd) orders magnetically down to 1.5 K. (C) 1998 American Institute of Physics.
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页码:7312 / 7314
页数:3
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