Magnetic ordering of Dy super(3+) ions in RbDy(WO sub(4)) sub(2) single crystal

The specific heat C(T) of the monoclinic RbDy(WO sub(4)) sub(2) crystal has been studied at very low temperatures 0.2 less than or equal to T less than or equal to 1.9 K and in magnetic fields 0 less than or equal to H less than or equal to 0.38 T. The Neel temperature was shown to be equal to T sub...

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Veröffentlicht in:Journal of low temperature physics 1998-03, Vol.110 (5-6), p.1003-1011
Hauptverfasser: Borowiec, M T, Dyakonov, V P, Jedrzejczak, A, Markovich, V I, Pavlyuk, A A, Szymczak, H, Zubov, E E, Zaleski, M
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container_end_page 1011
container_issue 5-6
container_start_page 1003
container_title Journal of low temperature physics
container_volume 110
creator Borowiec, M T
Dyakonov, V P
Jedrzejczak, A
Markovich, V I
Pavlyuk, A A
Szymczak, H
Zubov, E E
Zaleski, M
description The specific heat C(T) of the monoclinic RbDy(WO sub(4)) sub(2) crystal has been studied at very low temperatures 0.2 less than or equal to T less than or equal to 1.9 K and in magnetic fields 0 less than or equal to H less than or equal to 0.38 T. The Neel temperature was shown to be equal to T sub(N) identical with 0.818 plus or minus 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k identical with -0.798 K. The C(T) dependence below Neel temperature (0.5 T sub(N) < T < 0.99T sub(N)) is well described by 2D Ising model, whereas in the temperature region close above T sub(N) (1.01 T sub(N) < T < 2T sub(N)) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-T sub(N) diagrams for field H parallel a are in a reasonable agreement for simple quadratic lattice.
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The Neel temperature was shown to be equal to T sub(N) identical with 0.818 plus or minus 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k identical with -0.798 K. The C(T) dependence below Neel temperature (0.5 T sub(N) &lt; T &lt; 0.99T sub(N)) is well described by 2D Ising model, whereas in the temperature region close above T sub(N) (1.01 T sub(N) &lt; T &lt; 2T sub(N)) it can be described by neither 2D, nor 3D Ising model. 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subjects Magnetic field effects
Magnetization
Mathematical models
Single crystals
Specific heat of solids
title Magnetic ordering of Dy super(3+) ions in RbDy(WO sub(4)) sub(2) single crystal
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