首页> 外文期刊>Journal of Physics. Condensed Matter >SPIN-GLASS-LIKE BEHAVIOUR AND LOW-TEMPERATURE SPECIFIC HEAT OF AMORPHOUS ERXNI100-X RANDOM MAGNETIC ANISOTROPY SYSTEM
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SPIN-GLASS-LIKE BEHAVIOUR AND LOW-TEMPERATURE SPECIFIC HEAT OF AMORPHOUS ERXNI100-X RANDOM MAGNETIC ANISOTROPY SYSTEM

机译:非晶态ERXNI100-X随机磁各向异性系统的自旋玻璃行为和低温比热

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摘要

Spin-glass-like behaviour and low-temperature specific heat have been investigated for bulk amorphous ErxN100-x (x = 33, 50 and 80) alloys prepared by high-rate direct-current sputtering. The competition between ferromagnetic and antiferromagnetic interactions arising from the exchange fluctuations is negligibly small in this system, in contrast to that in amorphous Er-Cu alloys. The random magnetic anisotropy (RMA) suppresses the ferromagnetic coupling, resulting in a spin-glass-like state. The magnetization per Er atom becomes smaller with increasing Er content owing to the increase in the RMA. At the spin freezing temperature T-f the low-temperature specific heat exhibits a broad maximum, which becomes narrower with the decrease in Er content. It should be noted that the temperature at which the magnetic specific heat of the amorphous Er33Ni67 alloy reaches a maximum value coincides with the T-f determined by the alternating-current magnetic susceptibility measurement. The splitting of the ground state from J = 15/2 into a Kramers doublet is caused by the electrostatic field, being accompanied by a Schottky-type specific heat with a linear temperature dependence. The magnetic entropy at T-f is estimated to be about 45-60% of the theoretical value, being much larger than those for crystalline dilute spin-glass systems. Moreover, the plot of the magnetic specific heat versus T-3/2 is, linear at low temperatures. Therefore, it is considered that a ferromagnetic-like spin wave is excited, although its magnetic structure is not ferromagnetic. [References: 29]
机译:对于通过高速直流溅射制备的块状非晶ErxN100-x(x = 33、50和80)合金,已经研究了类似自旋玻璃的行为和低温比热。与非晶态Er-Cu合金相比,在该系统中,由交换波动引起的铁磁和反铁磁相互作用之间的竞争微不足道。随机磁各向异性(RMA)抑制了铁磁耦合,从而形成了类似自旋玻璃的状态。由于RMA的增加,随着Er含量的增加,每个Er原子的磁化变小。在旋转冻结温度T-f下,低温比热表现出较宽的最大值,随着Er含量的降低,该最大值变窄。应当注意,非晶态Er33Ni67合金的磁比热达到最大值的温度与通过交流磁化率测量确定的T-f一致。基态从J = 15/2分裂成Kramers双峰是由静电场引起的,同时伴随着线性肖特基型比热,其线性温度依赖性。据估计,T-f处的磁熵约为理论值的45-60%,比晶体稀自旋玻璃系统的磁熵大得多。此外,在低温下,磁比热与T-3 / 2的关系图是线性的。因此,尽管其磁性结构不是铁磁性的,但仍认为是激发了类似铁磁性的自旋波。 [参考:29]

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