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arXiv 1003.4096cond-mat.str-elcond-mat.mtrl-scicond-mat.quant-gas
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量子自旋电子中的磁振子配对

Magnon pairing in quantum spin nematic

M. E. Zhitomirsky, Hirokazu Tsunetsugu

摘要:

竞争的铁磁和反铁磁交换相互作用可能会导致在受抑量子磁体的高场相中形成束缚磁振子对。随着磁场的减小,磁振子对在传统的单磁振子不稳定性发生之前经历玻色凝聚。我们发展了一种分析方法来研究磁振子对凝聚体的零温性质,它是BCS超导体的玻色子模拟。用相干玻色子态表示凝聚体波函数,揭示了基态的自旋对称性,并允许计算各种静态性质。尖锐的准粒子激发被发现在一个小的有限间隙的π态。我们还预测了在高场的阻挫链材料LiCuVO 4中存在长程有序的自旋-自旋相。

英文摘要:

Competing ferro- and antiferromagnetic exchange interactions may lead to the formation of bound magnon pairs in the high-field phase of a frustrated quantum magnet. With decreasing field, magnon pairs undergo a Bose-condensation prior to the onset of a conventional one-magnon instability. We develop an analytical approach to study the zero-temperature properties of the magnon-pair condensate, which is a bosonic analog of the BCS superconductors. Representation of the condensate wave-function in terms of the coherent bosonic states reveals the spin-nematic symmetry of the ground-state and allows one to calculate various static properties. Sharp quasiparticle excitations are found in the nematic state with a small finite gap. We also predict the existence of a long-range ordered spin-nematic phase in the frustrated chain material LiCuVO4 at high fields.

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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