arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2003.02507cond-mat.str-el
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无限自旋1/2阶梯中的无隙和大量一维单重态色散通道-激发的无限准一维纠缠微扰理论

Gapless and Massive 1D Singlet Dispersion Channel in Infinite Spin-1/2 Ladders ---Infinite Quasi-1D Entanglement Perturbation Theory for Excitation

Lihua Wang, Aslam Parvej, D. ChangMo Yang, Kwang S. Kim

摘要:

推广了最近发展的无限准一维纠缠微扰理论,求解了无限准一维量子晶格中的元激发。激发态的波函数是通过优化团簇操作的叠加而变分确定的,每个团簇操作都是由一个格点块内的同时原位操作组成的,以平面波的形式叠加在基态上。相对于波数的激发能给出了基元激发的光谱。我们的方法是人工加宽自由,是适应各种准粒子图片。使用三重态谱,应用于$N=2, 4, 6, 8$和$10$的$\infty$ -by- $N$反铁磁自旋- $\frac{1}{2}$梯,证实了以前的报道,即存在量子尺寸跃迁,即晶格在有限的临界值$N_c=10$从准一维跃迁到二维.在$\left( π, π\right)$处的无质量三重态色散看到消失的能隙。我们的结果检测到的异常$\left(π,0\right)$在三重态谱,同意与宏观样品的非弹性中子散射测量。令人惊讶的是,我们的研究结果还揭示了一个无隙和大规模的一维单重态色散通道,这是远远低于三重态激发。然而,我们注意到,尺寸跃迁是由无质量三重态色散决定的。

英文摘要:

We solve for the elementary excitation in infinite quasi-1D quantum lattices by extending the recently developed infinite quasi-1D entanglement perturbation theory. The wave function of an excited state is variationally determined by optimizing superposition of cluster operation, each of which is composed of simultaneous on-site operation inside a block of lattice sites, on the ground state in a form of plane wave. The excitation energy with respect to the wave number gives the spectra for an elementary excitation. Our method is artificial broadening free and is adaptive for various quasi-particle pictures. Using the triplet spectrum, the application to $\infty$-by-$N$ antiferromagnetic spin-$\frac{1}{2}$ ladders for $N=2, 4, 6, 8$, and $10$ confirms a previous report that there is a quantum dimensional transition, namely, the lattice transits from quasi-1D to 2D at a finite critical value $N_c=10$. The massless triplet dispersion at $\left( π, π\right)$ sees a vanishing gap. Our results detect the anomaly at $\left(π,0\right)$ in the triplet spectrum, agreeing well with the inelastic neutron scattering measurement of a macroscopic sample. Surprisingly, our results also reveal a gapless and massive 1D singlet dispersion channel that is much lower than the triplet excitation. We note, however, the dimensional transition is determined by the massless triplet dispersion.

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