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57 Fe Probe Mössbauer Study of Magnetic Phase Transitions in MnP Phosphide
Journal of Experimental and Theoretical Physics ( IF 1.1 ) Pub Date : 2020-09-01 , DOI: 10.1134/s1063776120050027
A. A. Aslandukova , A. V. Sobolev , I. G. Silkin , I. V. Morozov , I. S. Glazkova , I. A. Presniakov

Abstract

57Fe Mössbauer studies of Mn0.99557Fe0.005P monophosphide have been performed in a wide temperature range including magnetic transitions at the points TC = 292 K and TN = 60 K, the former of which (at TC) is a transition from the paramagnetic to ferromagnetic phase and the latter (at TN) is a transition with the formation of a helical magnetic structure. The model interpretation of the Mössbauer spectra within the full hyperfine interaction Hamiltonian involves the features of the magnetic structure of undoped MnP phosphide. The analysis of spectra at T < TN has shown that it is necessary to take into account the magnetocrystalline anisotropy of the helical structure of MnP and the anisotropy of the hyperfine magnetic field Hhf on 57Fe nuclei. It has been found that a Bloch-type domain structure is formed in a ferromagnetic phase in the temperature range T0 < T < TC (T0 ≈ 119 K) and that two magnetic structures coexist in the temperature range of TN < T < T0. The analysis of the temperature dependence Hhf(T) within the molecular field theory including magnetostriction effects (Bean–Rodbell model) has indicated that the phase transitions at TN and TC are of the first and second orders, respectively. It has been established that the magnetic moments μFe undergo strong thermal fluctuations in the wide temperature range of T* < T < TC (T* ≈ 190 K).


中文翻译:

57 Fe探针Mössbauer研究MnP磷酸盐中的磁性相变

摘要

57个的Mn的Fe穆斯堡尔研究0.995 57的Fe 0.005 P磷化已经在很宽的温度范围内,包括在点磁转变被执行Ť Ç = 292 K和Ť Ñ = 60 K,其中前者的(在Ť Ç)是过渡从顺磁相到铁磁相,铁磁相(在T N处)是形成螺旋磁性结构的过渡。完全超精细相互作用哈密顿量内的Mössbauer光谱的模型解释涉及未掺杂MnP磷化物的磁性结构特征。T < T处的光谱分析N已经表明,有必要考虑MnP的螺旋结构的磁晶各向异性和57 Fe核上的超精细磁场H hf的各向异性。已经发现的是,在所述温度范围内的铁磁性相形成的布洛赫型结构域结构Ť 0 < Ť < Ť ÇŤ 0 ≈119 K),并且在该温度范围的两个磁结构并存Ť Ñ < Ť < T 0。温度依赖性H hfT)在包括磁致伸缩效应的分子场论中(Bean-Rodbell模型)表明,在T NT C处的相变分别为一阶和二阶。已经确定的是,磁矩μ的Fe在宽温度范围内的强经受热波动Ť * < Ť < Ť ÇŤ *≈190 K)。
更新日期:2020-09-01
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