EuxSr1- xS自旋玻璃在强磁场中的磁振子激发和比热

U. Krey
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引用次数: 6

摘要

在强磁场B(即B>3 t)条件下,计算了x=0.25、0.44和0.54的Eu x Sr 1−x S自旋玻璃的类磁振子激发态密度,发现在这些强磁场下,类磁振子激发态可以被视为非相互作用玻色子,直至远超过自旋玻璃冻结温度B=0的温度。由态密度计算出比热的磁性部分hc,不需要任何拟合参数。在3.6 T (6.6 T)的磁场中,当T在0.3 K到5 K (10 K)之间时,研究了准磁振子的激发,结果与最近的实验结果一致,当x= 0,25,0,44和0,54时,磁性强(B>3 T),准磁振子的性质与非相互作用的玻色子的性质一致,温度,转变,自旋,B=0。计算,无参数可调,关于磁振子和磁振子的密度
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Magnon excitations and the specific heat of EuxSr1- xS spin glasses in strong magnetic fields
The density of states of magnon-like excitations of Eu x Sr 1−x S spin glasses with x=0.25, 0.44 and 0.54 is calculated for very strong magnetic fields B, i.e. B>3 T. It is found that for these high fields the magnon-like excitations can be treated as non-interacting bosons up to temperatures far beyond the spin glass freezing temperature at B=0. From the density of states the magnetic part C H of the specific heat is calculated, without any fit-parameter. The results agree quantitatively with recent experiments, for T between 0.3 K and 5 K (10 K) in magnetic fields of 3.6 T (6.6 T) Etude des excitations de quasi-magnons dans ces composes pour x=0,25, 0,44 et 0,54 en champ magnetique intense (B>3 T). Traitement de ces quasi-magnons comme des bosons non interagissants bien au-dessous de la temperature de transition de verre de spin a B=0. Calcul, sans parametre ajustable, de la densite d'etats des magnons et de la chaleur massique magnetique
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