Abstract
Reentrant behavior to a spin glass state is discovered in the solid solution system CuCr1.5+0.5x Sb x0.5−0.5 x S 4 with x=0.34 and 0.4. The spin-glass transition temperature T f determined from the kink in the temperature dependence of the initial susceptibility in an alternating magnetic field depends on the measurement frequency ω. It is shown that the frequency dependence T f (ω) is a power-law function 1/ω=(1/ω0)[T f /( T f − T *)]zv with zv =7.7 for both compositions. For the composition with x =0.34 a maximum is observed near T * in the temperature dependence of the resistivity. These facts indicate that the transition from the spin glass to long-range magnetic order is a phase transition.
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References
L. I. Koroleva, Ja. A. Kessler, A. G. Odintsov et al., J. Magn. Magn. Mater. 140–144, 2015 (1995).
A. Z. Reznitskii, E. V. Sklyarov, L. F. Piskunova, and Z. F. Ushapovskii, Zapiski Vsesoyuz. Mineralogicheskogo Obshchestva 1, 57 (1989).
K. Binder and A. Young, Rev. Mod. Phys. 58, 801 (1986).
J. L. Tholence, Solid State Commun. 35, 113 (1980).
P. C. Hohenberg and B. L. Halperin, Rev. Mod. Phys. 49, 435 (1977).
A. T. Ogielski, Phys. Rev. B 32, 7384 (1985).
K. Binder and A. Young, Phys. Rev. B 29, 2864 (1984).
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Pis’ma Zh. Éksp. Teor. Fiz. 64, No. 4, 265–269 (25 August 1996)
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Belov, K.P., Virovets, T.V., Koroleva, L.I. et al. Phase transition from spin glass to long-range magnetic order in semiconductor spinels CuCr1.5+0.5x Sb0.5−0.5x S4 (x=0.34 and 0.4). Jetp Lett. 64, 292–297 (1996). https://doi.org/10.1134/1.567185
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DOI: https://doi.org/10.1134/1.567185