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On the dynamics of the reentrant spin-glass state of the Fe_(100-x)Zr_x(x= 9,10) amorphous alloys

机译:Fe_(100-x)Zr_x(x = 9,10)非晶合金的重入自旋玻璃态动力学

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摘要

Low temperature magnetization (M) and ac susceptibility (x_(ac)) data were used to investigate the reentrant spin-glass state in lengths of melt-spun ribbons of Fe_(100-x)Zr_x(x = 9, 10) amorphous alloys. The temperature range investigated was from 2 to 300 K, while the applied magnetic field H was varied in the range of ±85 kOe. The magnetic properties were found to be strongly influenced by the sample composition despite the fact that the amount of Fe varies by 1 at. %. For instance, the Curie temperature (T_C) is reduced from 232.5 K to 213.0 K with decreasing Fe concentration, while M for the lower Fe concentration, measured at the highest applied magnetic field (H=85 kOe) was nearly double the value for that of the higher; the coercivity in the ferromagnetic regime is reduced by a factor close to five when x is increased from 9 at. % to 10 at. %. The ac susceptibility measured for frequencies f in the range of 10-10~4 Hz showed a sharp drop in the magnitude of the in-phase contribution (x′_(ac)) and a peak at the out-of-phase component (x″_(ac)), which shifts to higher temperatures with increasing values of f. The Voguel-Fulcher law applied to the x″_(ac) data yielded an activation energy E_a/k_B = 21.3K (40.1 K), the glassy temperature T_G = 15.5K (38.2K), and a relaxation time τ_0 = 9.1 × 10~(-7) s (8.3 × 10~(-7) s), for the sample with x = 10 (x = 9). A plot of x″_(ac) vs x′_(ac) for a broad range of T and f yielded a broad maximum near the glassy temperature T_G for both sample concentrations.
机译:低温磁化(M)和磁化率(x_(ac))数据用于研究Fe_(100-x)Zr_x(x = 9,10)非晶态合金的熔纺带长度内的折返自旋玻璃态。研究的温度范围为2至300 K,而施加的磁场H在±85 kOe的范围内变化。尽管铁的量变化了1 at,但发现磁性能受样品组成的强烈影响。 %。例如,随着铁浓度的降低,居里温度(T_C)从232.5 K降低到213.0 K,而在最高磁场(H = 85 kOe)下测得的较低铁浓度的M几乎是该值的两倍。较高的当x从9 at增加时,铁磁态的矫顽力降低了近五倍。 %至10 at。 %。在10-10〜4 Hz范围内的频率f下测得的ac磁化率显示出同相贡献(x'_(ac))的幅度急剧下降,并且在异相分量处达到峰值( x” _(ac)),随着f的增加,温度会升高。应用于x''_(ac)数据的Voguel-Fulcher法则产生活化能E_a / k_B = 21.3K(40.1 K),玻璃化温度T_G = 15.5K(38.2K)和弛豫时间τ_0= 9.1×对于x = 10(x = 9)的样本,10〜(-7)s(8.3×10〜(-7)s)。对于两种样品浓度,在宽的T和f范围内绘制x''_(ac)与x'_(ac)的图在玻璃化温度T_G附近产生了宽的最大值。

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  • 来源
    《Journal of Applied Physics》 |2015年第3期|17E124.1-17E124.4|共4页
  • 作者单位

    Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife-Pernambuco, Brazil;

    Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife-Pernambuco, Brazil;

    School of Physics and Astronomy, University of Minnesota, Minneapolis, Minnesota 55455, USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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