Neutron-diffraction studies of R5Rh4Ge10 (R = Tb, Ho, Er) compounds

被引:0
|
作者
M. Kolenda
M. Hofmann
J. Leciejewicz
B. Penc
A. Szytuła
机构
[1] Institute of Physics,
[2] Jagellonian University,undefined
[3] ul. Reymonta 4,undefined
[4] 30-059 Kraków,undefined
[5] Poland,undefined
[6] Berlin Neutron Scattering Center,undefined
[7] Hahn-Meitner Institut,undefined
[8] Glienicker Strasse 100,undefined
[9] 14109 Berlin,undefined
[10] Germany,undefined
[11] Institute of Nuclear Chemistry and Technology,undefined
[12] 03-169 Warszawa,undefined
[13] Poland,undefined
来源
Applied Physics A | 2002年 / 74卷
关键词
PACS: 61.12.-q; 75.25.+z; 75.50.Ee;
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学科分类号
摘要
Neutron-diffraction patterns recorded in the paramagnetic state confirmed that R5Rh4Ge10 (R = Tb, Ho, Er) compounds exhibit the tetragonal Sc5Co4Si10 (P4/mbm space group)-type of crystal structure. In this structure the rare-earth atoms R occupy three nonequivalent atomic positions. The low-temperature neutron-diffraction data confirm the change of the magnetic structure at Tt=3.8 and at the Néel temperature TN=11.5 K for R = Tb, at TN=7 K for R = Ho, and at Tt=4.2 K and TN=5.5 K for R = Er. In all these compounds the rare-earth moments form complex antiferromagnetic structures: collinear in the case of Tb and Ho compounds, sine-wave-modulated for Er5Rh4Ge10 with the wave vector k= \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\frac\Box1\Box\Box4\Box$\end{document},\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\frac\Box1\Box\Box4\Box$\end{document},0 for 1.5 K<T<4.2 K and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\frac\Box1\Box\Box3\Box$\end{document},\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\frac\Box1\Box\Box3\Box$\end{document},0 for 4.2 K up to TN. The magnetic moment values are different in different sublattices.
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页码:s769 / s771
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