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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Magnetic excitations in the Zn-Mg-Tb icosahedral quasicrystal: An inelastic neutron scattering study
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Magnetic excitations in the Zn-Mg-Tb icosahedral quasicrystal: An inelastic neutron scattering study

机译:Zn-Mg-Tb二十面体准晶体中的磁激发:非弹性中子散射研究

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Low-temperature spin dynamics in the face-centered-icosahedral Zn-Mg-Tb quasicrystal has been investigated by inelastic neutron scattering around its spin-glass-like freezing temperature (T_f approx = 5.8 K). A single broad inelastic peak, centered at h ω approx = 2.5 meV, was observed in the inelastic scattering spectrum at temperatures ranging from the base temperature up to ~ 20 K. The inelastic peak energy is Q independent, whereas the peak intensity shows weak Q dependence, which is qualitatively similar to that observed for the elastic diffuse scattering. The inelasticity of spin excitations is hardly seen in canonical spin glasses and thus is a distinct feature of the Zn-Mg-Tb quasicrystal. We argue, with an aide of numerical simulation, that this broad inelastic peak can be interpreted as localized collective fluctuations of short-range-ordered spins in a dodecahedral spin cluster. In a much lower-energy region (hω < 0.8 meV), we observed a strong quasielastic signal, appearing only above T_f; its peak width decreases as the temperature is lowered and vanishes at T_f. It is thus evident that the quasielastic signal corresponds to a slow spin dynamics that freezes at the macroscopic freezing temperature. The coexistence of the inelastic peak and quasielastic signal suggests that the short-range order in the single cluster is robustly formed but is dynamic for T_f < T < 20 K. The macroscopic freezing at T_f is, thus, attributed to a random freezing of spin-cluster fluctuations.
机译:通过非弹性中子散射,在围绕其中心的二十面体Zn-Mg-Tb准晶体中的低温自旋动力学,该中子散射类似于自旋玻璃的凝固温度(T_f约= 5.8 K)。在从基础温度到约20 K的温度范围内的非弹性散射谱中,观察到一个中心为hω的宽泛的非弹性峰,约为2.5 meV。非弹性峰能量与Q无关,而峰强度却显示弱Q依赖关系,在质量上与弹性扩散散射所观察到的相似。在标准自旋玻璃中几乎看不到自旋激发的非弹性,因此是Zn-Mg-Tb准晶体的一个明显特征。我们认为,在数值模拟的帮助下,这个宽泛的非弹性峰可以解释为十二面体自旋簇中短程有序自旋的局部集体波动。在低得多的能量区域(hω<0.8 meV),我们观察到了强烈的准弹性信号,仅在T_f以上出现;其峰宽随温度降低而减小,并在T_f处消失。因此很明显,准弹性信号对应于在宏观冻结温度下冻结的慢自旋动力学。非弹性峰和准弹性信号的共存表明,单个簇中的短程有序形成,但是对于T_f

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