Oscillations of the Hall Resistivity in Natural Single Crystals of Pyrrhotite Associated with the Orientation of the Elementary Magnetic Moments of Fe Atoms

S. Sakkopoulos, E. Vitoratos
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Abstract

The Hall resistivity of natural single crystals of pyrrhotite Fe7S8 exhibits oscillations with the inverse external magnetic field 1/B at temperature 77 K and B up to 0.73 Tesla. This resembles phenomena due to Landau quantization of the carriers demanding very pure samples, temperatures near 4 K and magnetic fields of several Tesla. However, none of these requirements is met in the experiments. The oscillations appear only when there is orientation of the elementary magnetic moments of Fe atoms, which happens when B is parallel to the c‐plane at 77 K. At room temperature with the orientation destroyed by the thermal agitation and for B parallel to the c‐axis along which the alignment of the Fe magnetic moments is negligible, the oscillations disappear. According to the s–d model proposed for heavily doped magnetic semiconductors, defects and impurities produce large local fluctuations of carrier concentrations. These through the strong s–d exchange interaction between the carriers and the lattice magnetic moments of Fe establish variations of local magnetization. These constitute scattering centers which are enforced for certain values of B, though for others weaken giving the oscillatory behavior of the Hall resistivity.
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磁黄铁矿天然单晶霍尔电阻率振荡与铁原子基本磁矩取向的关系
磁黄铁矿Fe7S8天然单晶在77 K和0.73 Tesla温度下,霍尔电阻率随反外磁场1/B的变化而振荡。这类似于载流子的朗道量子化现象,需要非常纯净的样品,接近4 K的温度和几个特斯拉的磁场。然而,这些要求在实验中都没有得到满足。只有当铁原子的基本磁矩有取向时才会出现振荡,当B平行于77 K的c -平面时才会出现振荡。在室温下,当取向被热搅拌破坏时,当B平行于c轴时,铁磁矩沿c轴的排列可以忽略不计,振荡消失。根据高掺杂磁性半导体的s-d模型,缺陷和杂质会产生较大的载流子浓度局部波动。这些通过载流子和铁晶格磁矩之间的强s-d交换相互作用建立了局部磁化的变化。这些构成散射中心,在某些B值下,散射中心被加强,而在其他B值下,散射中心减弱,产生霍尔电阻率的振荡行为。
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