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arXiv 2012.01669cond-mat.str-elcond-mat.mtrl-sci
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量子临界点附近磁体的全矩和规则

Total Moment Sum Rule for Magnets in the Vicinity of Quantum Critical Point

Masashige Matsumoto

摘要:

在量子磁系统的有序相中,在量子临界点附近可以存在纵向和横向激发模。在扩展的自旋波理论的基础上导出了这种系统的总矩和规则,其中考虑了纵向和横向磁激励。和规则被分解成弹性,一个磁振子,和两个磁振子组件。该公式适用于具有纵模的自旋系统,例如具有易平面型单离子各向异性的$S=1$系统和自旋二聚体系统。这一结果有助于我们对中子非弹性散射测量数据的分析和理解。

英文摘要:

It is known that the longitudinal and transverse excitation modes can exist in the vicinity of a quantum critical point in the ordered phase of quantum magnetic systems. The total moment sum rule for such systems is derived on the basis of the extended spin-wave theory, where both longitudinal and transverse magnetic excitations are taken into account. The sum rule is resolved into elastic, one-magnon, and two-magnon components. The formulation is applicable to spin systems with the longitudinal mode, such as $S=1$ systems with single-ion anisotropy of easy-plane type and spin dimer systems. The result helps us analyze and understand measured data of inelastic neutron scattering.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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