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1/1近似物Ag(50)In(36)Gd(14)与二十面体准晶体Ag(50)In(36)Gd(14)磁性的比较研究。

A comparative study of the magnetic properties of the 1/1 approximant Ag(50)In(36)Gd(14) and the icosahedral quasicrystal Ag(50)In(36)Gd(14).

作者信息

Wang P, Stadnik Z M, Al-Qadi K, Przewoźnik J

机构信息

Department of Physics, University of Ottawa, Ottawa, ON, K1N 6N5, Canada.

出版信息

J Phys Condens Matter. 2009 Oct 28;21(43):436007. doi: 10.1088/0953-8984/21/43/436007. Epub 2009 Oct 8.

Abstract

We report on measurements of the dc and ac magnetic susceptibility, (155)Gd Mössbauer spectra, and specific heat of the 1/1 approximant Ag(50)In(36)Gd(14), and of the ac magnetic susceptibility of the icosahedral quasicrystal Ag(50)In(36)Gd(14). These alloys are shown to be spin glasses. For the icosahedral quasicrystal Ag(50)In(36)Gd(14), spin freezing occurs at T(f) = 4.3 K, and the frequency dependence of T(f) is well accounted for by the Vogel-Fulcher and power laws. Spin freezing in the 1/1 approximant Ag(50)In(36)Gd(14) occurs in two stages: at T(f(1)) = 3.7 K, Gd spins develop short-range correlations but continue to fluctuate, and then long-range freezing is achieved at T(f(2)) = 2.4 K. The frequency dependences of T(f(1)) and T(f(2)) can be accounted for by means of the Vogel-Fulcher law and the critical slowing down dynamics. It is shown that the spin freezing in both alloys is a nonequilibrium phenomenon rather than a true equilibrium phase transition. The (155)Gd Mössbauer spectra of the 1/1 approximant Ag(50)In(36)Gd(14) confirm that the Gd spins are frozen at 1.5 K and are fluctuating at 4.6 K. The magnetic specific heat exhibits a maximum at a temperature that is 30% larger than T(f(1)), but the temperature derivative of the magnetic entropy peaks at T(f(1)). The Debye temperature of the 1/1 approximant Ag(50)In(36)Gd(14) is 199(1) K as determined from the Mössbauer data, and 205(2) K as determined from the specific heat data.

摘要

我们报告了1/1近似物Ag(50)In(36)Gd(14)的直流和交流磁化率、(155)Gd穆斯堡尔谱以及比热的测量结果,以及二十面体准晶体Ag(50)In(36)Gd(14)的交流磁化率。这些合金被证明是自旋玻璃。对于二十面体准晶体Ag(50)In(36)Gd(14),自旋冻结发生在T(f)=4.3 K,并且T(f)的频率依赖性可以通过Vogel-Fulcher定律和幂律很好地解释。1/1近似物Ag(50)In(36)Gd(14)中的自旋冻结分两个阶段发生:在T(f(1))=3.7 K时,Gd自旋形成短程关联但继续波动,然后在T(f(2))=2.4 K时实现长程冻结。T(f(1))和T(f(2))的频率依赖性可以通过Vogel-Fulcher定律和临界慢化动力学来解释。结果表明,两种合金中的自旋冻结都是非平衡现象,而不是真正的平衡相变。1/1近似物Ag(50)In(36)Gd(14)的(155)Gd穆斯堡尔谱证实,Gd自旋在1.5 K时被冻结,在4.6 K时波动。磁比热在比T(f(1))高30%的温度处出现最大值,但磁熵的温度导数在T(f(1))处达到峰值。根据穆斯堡尔数据确定,1/1近似物Ag(50)In(36)Gd(14)的德拜温度为199(1) K,根据比热数据确定为205(2) K。

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