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arXiv 2301.13596cond-mat.str-el
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三角晶格反铁磁体中分数激发的约束

Confinement of fractional excitations in a triangular lattice antiferromagnet

L. Facheris, S. D. Nabi, A. Glezer Moshe, U. Nagel, T. Rõõm, K. Yu. Povarov, J. R. Stewart, Z. Yan, A. Zheludev

AI总结:

本研究通过高分辨率光谱揭示三角晶格反铁磁体Cs$_2$CoBr$_4$的磁激发并非连续谱,而是类似“塞曼阶梯”的束缚态,即分数激发被约束为有限宽度扭结,并阐明了其二维特性。

摘要:

利用高分辨率中子和太赫兹光谱研究了Cs$_2$CoBr$_4$的磁激发谱,这是一种具有近XY型各向异性的畸变三角晶格反铁磁体。先前被认为是宽激发连续谱的现象[Phys. Rev. Lett. 129, 087201 (2022)]被证明是一系列色散束缚态,类似于准一维伊辛系统中的“塞曼阶梯”。在波矢处,当链间相互作用在平均场水平上抵消时,它们确实可以被解释为单链中束缚的有限宽度扭结。在布里渊区的其他位置,它们真正的二维结构和传播得以揭示。

英文摘要:

High-resolution neutron and THz spectroscopies are used to study the magnetic excitation spectrum of Cs$_2$CoBr$_4$, a distorted-triangular-lattice antiferromagnet with nearly XY-type anisotropy. What was previously thought of as a broad excitation continuum [Phys. Rev. Lett. 129, 087201 (2022)] is shown to be a series of dispersive bound states reminiscent of "Zeeman ladders" in quasi-one-dimensional Ising systems. At wave vectors where inter-chain interactions cancel at the Mean Field level, they can indeed be interpreted as bound finite-width kinks in individual chains. Elsewhere in the Brillouin zone their true two-dimensional structure and propagation are revealed.

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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