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Quasiparticle vanishing driven by geometrical frustration

机译:几何挫折驱动准粒子消失

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We investigate the single hole dynamics in the triangular t-J model. We study the structure of the hole spectral function, assuming the existence of a 120° magnetic Neel order. Within the self-consistent Born approximation (SCBA) there is a strong momentum and t sign dependence of the spectra, related to the underlying magnetic structure and the particle-hole asymmetry of the model. For positive t, and in the strong coupling regime, we find that the low-energy quasiparticle excitations vanish outside the neighborhood of the magnetic Goldstone modes; while for negative t the quasiparticle excitations are always well defined. In the latter, we also find resonances of magnetic origin whose energies scale as (J/t)~(2/3) and can be identified with string excitations. We argue that this complex structure of the spectra is due to the subtle interplay between magnon-assisted and free-hopping mechanisms. Our predictions are supported by an excellent agreement between the SCBA and the exact results on finite-size clusters. We conclude that the conventional quasiparticle picture can be broken by the effect of geometrical magnetic frustration.
机译:我们研究了三角形t-J模型中的单孔动力学。假设存在120°磁性Neel阶,我们研究空穴光谱函数的结构。在自洽Born逼近(SCBA)中,光谱具有很强的动量和t符号依赖性,与基础磁性结构和模型的粒子-孔不对称性有关。对于正t,在强耦合状态下,我们发现低能准粒子激发在磁性戈德斯通模态附近消失了。对于负t,准粒子激励总是定义良好的。在后者中,我们还发现了磁性原点的共振,其能量尺度为(J / t)〜(2/3),可以通过弦激励来识别。我们认为,频谱的这种复杂结构是由于磁振辅助和自由跳跃机制之间的微妙相互作用。我们的预测得到了SCBA与有限大小簇的精确结果之间的良好协议的支持。我们得出的结论是,常规的准粒子图像可能会由于几何磁阻效应而被破坏。

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