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Magnetic properties of a GdCr3(BO3)4 single crystal

A. N. BludovB.I. Verkin Institute for Low Temperature Physics and Engineering B.I., NAS of Ukraine , 47 Nauky Ave., Kharkiv 61103, UkraineYu. A. SavinaB.I. Verkin Institute for Low Temperature Physics and Engineering B.I., NAS of Ukraine , 47 Nauky Ave., Kharkiv 61103, UkraineВ. А. ПащенкоB.I. Verkin Institute for Low Temperature Physics and Engineering B.I., NAS of Ukraine , 47 Nauky Ave., Kharkiv 61103, UkraineS. L. GnatchenkoB.I. Verkin Institute for Low Temperature Physics and Engineering B.I., NAS of Ukraine , 47 Nauky Ave., Kharkiv 61103, UkraineV. V. MaltsevM.V. Lomonosov Moscow State University , Moscow 119991, RussiaN. N. KuzminM.V. Lomonosov Moscow State University , Moscow 119991, RussiaΝ. I. LeonyukM.V. Lomonosov Moscow State University , Moscow 119991, Russia
2018en
ABI

Аннотация

The temperature dependence of the magnetic susceptibility χ (T) of the GdCr3(BO3)4 single crystal was studied in the temperature range of 2–300 K for two orientations of the external magnetic field: H ǁ c and H ± c. It was established that gadolinium chromium borate is ordered antiferromagnetically at TN = 7 K. It was found that, at T > 10 K, the magnetic properties of the crystal are isotropic, which is characteristic of the pure spin states of Cr3+ and Gd3+ ions. It was demonstrated that the magnetic susceptibility χ(T) of the GdCr3(BO3)4 compound at T > TN is well described by a one-dimensional spin model for a system of ferromagnetic chains of Cr3+ ions with ferromagnetic exchange 2J/k = −13.6 K and antiferromagnetic interchain interaction of 2J′/k = + 0.72 K. The gadolinium subsystem is antiferromagnetically biased due to the exchange f-d-interaction, which gives θGd=−2.8K. It was assumed that the GdCr3(BO3)4 compound is an antiferromagnet with “easy-plane” type anisotropy in the magnetically ordered state.

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