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Magnetic Properties of Spinel FeCr\(_{2}\)S\(_{4}\) in High Magnetic Field

We studied temperature and magnetic field dependence of magnetization, \(M(T)\) and \(M(B)\), on thiospinel FeCr\(_{2}\)S\(_{4}\). We observed a step-like anomaly at \(T_{OO} \sim\) 9 K for \(M\)(\(T\)) attributed to an orbital order transition in magnetic field 0 \(< B \leq\) 7 T. Furthermore, a...

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Bibliographic Details
Published in:arXiv.org 2011-06
Main Authors: Ito, Masakazu, Nagi, Yuji, Kado, Naotoshi, Urakawa, Shinpei, Ogawa, Takuro, Kondo, Akihiro, Koyama, Keiichi, Watanabe, Kazuo, Kindo, Koichi
Format: Article
Language:English
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Summary:We studied temperature and magnetic field dependence of magnetization, \(M(T)\) and \(M(B)\), on thiospinel FeCr\(_{2}\)S\(_{4}\). We observed a step-like anomaly at \(T_{OO} \sim\) 9 K for \(M\)(\(T\)) attributed to an orbital order transition in magnetic field 0 \(< B \leq\) 7 T. Furthermore, also for \(M\)(\(B\)), an step-like anomaly appears at \(B_{c} \sim\) 5.5 T below \(T_{OO}\). This suggests an existence of a magnetic phase boundary at \(B_{c}\) in \(T < T_{OO}\). Because the anomaly at \(B_{c}\) of \(M(B)\) exists in the orbital ordered phase, the spin structure of FeCr\(_{2}\)S\(_{4}\) in \(T\
ISSN:2331-8422
DOI:10.48550/arxiv.1106.1248