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Investigation of the Itinerant Electron Ferromagnetism of Ni2+xMnGa1−x and Co2VGa Heusler Alloys

机译:Ni2 + xMnGa1-x和Co2VGa Heusler合金的流动电子铁磁性的研究

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摘要

Experimental investigations into the field dependence of magnetization and temperature dependences of magnetic susceptibility in Ni2+xMnGa1−x (x = 0.00, 0.02, 0.04) and Co2VGa Heusler alloy ferromagnets were performed following the spin fluctuation theory of itinerant ferromagnetism, called as “Takahashi theory”. We investigated the magnetic field dependence of magnetization at the Curie temperature TC, which is the critical temperature of the ferromagnetic–paramagnetic transition, and also at T = 5 K, which concerns the ground state of the ferromagnetic state. The field dependence of the magnetization was analyzed by means of the H vs. M5 dependence, and the field dependence of the ground state at 5 K was investigated by means of an Arrott plot (H/M vs. M2) according to the Takahashi theory. As for Ni2+xMnGa1−x, the spin fluctuation parameter in k-space (momentum space, TA) and that in energy space (T0) obtained at TC and 5 K were almost the same. On the contrary, as for Co2VGa, the H vs. M5 dependence was not shown at TC. We obtained TA and T0 by means of an Arrott plot at 5 K. We created a generalized Rhodes–Wohlfarth plot of peff/pS versus TC/T0 for the other ferromagnets. The plot indicated that the relationship between peff/pS and T0/TC followed Takahashi’s theory. We also discussed the spontaneous magnetic moment at the ground state, pS, which was obtained by an Arrott plot at 5 K and the high temperature magnetic moment, pC, at the paramagnetic phase. As for the localized ferromagnet, the pC/pS was 1. As for weak ferromagnets, the pC/pS was larger than 1. In contrast, the pC/pS was smaller than 1 by many Heusler alloys. This is a unique property of Heusler ferromagnets. Half-metallic ferromagnets of Co2VGa and Co2MnGa were in accordance with the generalized Rhodes–Wohlfarth plot with a km around 1.4. The magnetic properties of the itinerant electron of these two alloys appeared in the majority bands and was confirmed by Takahashi’s theory.
机译:Ni2 + xMnGa1-x(x = 0.00,0.02,0.04)和Co2VGa Heusler合金铁磁体的磁化场依赖性和磁化率的温度依赖性是根据流动铁磁性的自旋涨落理论(称为“高桥理论”)进行的”。我们研究了居里温度TC(即铁磁-顺磁转变的临界温度)以及T = 5 K(涉及铁磁态的基态)时磁化强度的磁场依赖性。利用H对M 5 的依赖性分析了磁化强度的场相关性,并通过Arrott图研究了5 K时基态的场相关性(H / M对M 2 )。对于Ni 2 + xMnGa 1-x,在TC和5K下获得的k空间(动量空间,TA)和能量空间(T0)中的自旋涨落参数几乎相同。相反,对于Co2VGa,在 T C中未显示H对 M 5 的依赖性。我们通过在5 K处的Arrott图获得了 T A和 T 0。我们创建了 p eff /的广义Rhodes-Wohlfarth图对于其他铁磁体, p S与 T C / T 0 。该图表明 p eff / p S T < sub> 0 / T C 遵循高桥的理论。我们还讨论了基态的自发磁矩 p S ,这是通过5 K的Arrott图和高温磁矩 p获得的。 C ,处于顺磁相。对于局部铁磁体, p C / p S 为1。对于弱铁磁体, p C / p S em> p C / p S 大于1。相反, p <许多Heusler合金的sub> C / p S 小于1。这是赫斯勒铁磁体的独特属性。 Co 2 VGa和Co 2 MnGa的半金属铁磁体符合广义Rhodes-Wohlfarth图,其 k m 在1.4左右。这两种合金的巡回电子的磁性都出现在多数能带中,并由高桥理论证实了这一点。

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