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arXiv 1602.01679cond-mat.str-el
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一维量子系统中含时关联函数的边界与体行为

Boundary versus bulk behavior of time-dependent correlation functions in one-dimensional quantum systems

I. S. Eliëns, F. B. Ramos, J. C. Xavier, R. G. Pereira

摘要:

在低能近似下研究了零温下反射边界对一维量子流体含时响应的影响。我们的分析是基于非线性Luttinger液体的有效移动杂质模型的开放边界条件的情况下的扩展。对于可积模型,我们表明,边界自相关振荡作为时间的函数与相应的散装自相关相同的频率。该频率可以被识别为基本激励的频带边缘。振荡的振幅衰减的幂律与不同的指数在边界和在散装,但边界和散装指数是由相同的耦合常数在移动杂质模型。对于不可积的模型,我们认为,幂律衰减的振荡是通用的自相关的散装,但变成一个指数衰减的边界。此外,在一般情况下,有一个非普遍的移动的边界频率相比,散装激发的带边。我们的有效场论的预测与含时密度矩阵重整化群(tDMRG)获得的数值结果进行了比较可积和不可积的临界自旋$S$链与$S=1/2$,$1$和$3/2$。

英文摘要:

We study the influence of reflective boundaries on time-dependent responses of one-dimensional quantum fluids at zero temperature beyond the low-energy approximation. Our analysis is based on an extension of effective mobile impurity models for nonlinear Luttinger liquids to the case of open boundary conditions. For integrable models, we show that boundary autocorrelations oscillate as a function of time with the same frequency as the corresponding bulk autocorrelations. This frequency can be identified as the band edge of elementary excitations. The amplitude of the oscillations decays as a power law with distinct exponents at the boundary and in the bulk, but boundary and bulk exponents are determined by the same coupling constant in the mobile impurity model. For nonintegrable models, we argue that the power-law decay of the oscillations is generic for autocorrelations in the bulk, but turns into an exponential decay at the boundary. Moreover, there is in general a nonuniversal shift of the boundary frequency in comparison with the band edge of bulk excitations. The predictions of our effective field theory are compared with numerical results obtained by time-dependent density matrix renormalization group (tDMRG) for both integrable and nonintegrable critical spin-$S$ chains with $S=1/2$, $1$ and $3/2$.

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