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spin-glass phase
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  自旋玻璃相
     Based on a Core-Shell model and the existence of spin-glass phase at the grain boundaries, we explained the observed resistance aging result and why our sample follows the stretched exponential law.
     利用Core-Shell模型以及自旋玻璃相的存在对观察到的时效行为及拟合结果进行了解释.
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  “spin-glass phase”译为未确定词的双语例句
     The temperature dependence of magnetization of amorphous Fe 77 Cr 13 Zr 10 alloy have been measured in the temperation range 1.5 to 300K. The results indicate:it is affected by the values of magenetic-field and there is a spin-glass phase in low temperature.
     测量了非晶态Fe77Cr13Zr10合金的磁化强度的温度关系,结果表明:这一关系受磁场大小的影响;
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  相似匹配句对
     ON THE ELECTRONIC SPIN
     关于电子自旋两则
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     The Power of Spin
     旋转的力量
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     THREE-SPIN THEORY
     三旋理论(Ⅱ)
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     F-SPIN BREAKING IN IBM
     相互作用玻色子模型中的F旋破缺
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     Is SrRuO_3 Spin Glass
     SrRuO_3是否为自旋玻璃(英文)
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  spin-glass phase
We consider the random energy model, where in the spin-glass phase, magnetization falls off exponentially as the volume increases.
      
Finite-volume corrections to magnetization in the spin-glass phase of the Derrida model
      
The degree of connectivity at which, for given noise, the transition from the ferromagnetic to the spin-glass phase occurs is found.
      
For copper oxides with impurities in which the nests are distributed in accordance with a random law and frozen the concentration of impurities at which an antiferromagnet-spin-glass phase transition occurs has been calculated.
      
The occurrence of the spin-glass phase in weak magnetic fields is demonstrated.
      
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Low-field magnetic susceptibility of the diluted magnetic semiconductors Zn_(1-x)Mn_(x~-) Se was measured between 4.2 and 30 K for the Mn concentration range 0.1≤x≤0.50 using SQUID magnetometer. When x≥0.30, the system shows a spin-glass transition in the above temperature range, as evidenced by a somewhat rounded cusp in the susceptibility. The transition temperature of spin-glass is as follow: x=0.30, T_f=10.5 K; x=0.40, T(?)=16.0 K; x=0.50, T_f=19.5 K. The phase diagrams for the boundary...

Low-field magnetic susceptibility of the diluted magnetic semiconductors Zn_(1-x)Mn_(x~-) Se was measured between 4.2 and 30 K for the Mn concentration range 0.1≤x≤0.50 using SQUID magnetometer. When x≥0.30, the system shows a spin-glass transition in the above temperature range, as evidenced by a somewhat rounded cusp in the susceptibility. The transition temperature of spin-glass is as follow: x=0.30, T_f=10.5 K; x=0.40, T(?)=16.0 K; x=0.50, T_f=19.5 K. The phase diagrams for the boundary of the paramagnetic and the spin-glass phases are obtained for this system. The difference of spin-glass transition temperature between Zn_(1-x)Mn_x Se and Cd_(1-x)MnxSe is discussed. It is found that for any given Mn concentration x the spin-glass transition temperature T_f, of Zn_(1-x)MnxSe is higher than that of Cd_(1-x)Mn_xSe.

用超导量子干涉器(SQUID)磁强计对稀释磁性半导体Zn_(1-x)Mn_xSe(0.1≤x≤0.50)的低温低场直流磁化率作了测量,测量温度从4.2K到30K,测量磁场为15Oe。当x≥0.30时,从磁化率-温度曲线的浑圆峰值,观察到了自旋玻璃的转变。自旋玻璃的转变温度T_f,对x=0.30,0.40,0.50,分别为10.5K,16K,19.5K。给出了顺磁相和自旋玻璃相的相图。比较了Zn_(1-x)Mn_xSe和Cd_(1-x)Mn_xSe的自旋玻璃转变温度,发现对同样的Mn离子浓度,Zn_(1-x)Mn_xSe的T_f高于Cd_(1-x)Mn_xSe的T_f,用交换作用的理论作了讨论。

The magnetic properties of the spin glass La FeyNis-y (0.5≤y≤1.1) are reported. The spin freezing temperatures, Tf, in these alloys have been measured. It is observed that at lower temperatures there is a transition from the paramagnetic (PM) to the ferromagnetic (FM) phase for y≤0.9 and the Fe-content dependence of the freezing temperature is approximately linear. There is a transition from the PM to the FM and from the FM to spin glass phase for y≤1.0

本文报道了金属间化合物LaFe_yNi_(5-y)(0.5≤y≤1.1)的自旋玻璃特性。测定了样品的自旋玻璃冻结温度T_f。y≤0.9时,在一定温度下,样品中发生顺磁-自旋玻璃转变,T_f近似为y的线性函数,y≥1.0时,材料将发生顺磁-铁磁-自旋玻璃转变。

An effective-field theory and an infinite-ranged random interaction Ising model are used to investigate the thermodynamic parameters of the spin glass phase with random field.

本文应用有效场理论和长程无规相互作用Ising型,讨论了S=1/2无规场自旋玻璃相的热力学参量。

 
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