论文标题
疾病对稻米模型中拓扑电荷抽水的影响
Effect of disorder on topological charge pumping in the Rice-Mele model
论文作者
论文摘要
超低量子气体的最新实验成功地实现了光学晶格中整数定量的拓扑电荷泵。在这一进步的动机下,我们研究了静态障碍对拓扑泵的影响。我们专注于自由无旋转费物的半充满水稻模型,并考虑随机对角线障碍。在瞬时,我们计算了极化,纠缠频谱和局部Chern标记。作为第一个主要结果,我们得出的结论是,空间融合的局部Chern标记最适合定量确定无序系统中拓扑转换。在时间依赖的模拟中,我们使用时间集成电流在缓慢定期驱动的系统中获得泵送电荷。作为第二个主要结果,我们观察并表征了量化电荷泵的疾病驱动的故障。静态与时间相关的计算泵电荷的方式之间有着极好的一致性。拓扑转变很好地发生在所有状态都位于给定系统大小上的状态下,因此与哈密顿特征态的离域定位跃迁不息息相关。为了实现个体障碍,对于参数发生了量化泵送的分解,其中频谱散装间隙从干净系统的带隙封闭,导致全球无间隙的光谱。作为第三个主要结果以及对有限尺寸系统的分析,我们表明,散装间隙的平均障碍严重高估了量化泵送的稳定性。一个更好的估计是能量间隙分布的典型值,也称为分布模式。
Recent experiments with ultracold quantum gases have successfully realized integer-quantized topological charge pumping in optical lattices. Motivated by this progress, we study the effects of static disorder on topological Thouless charge pumping. We focus on the half-filled Rice-Mele model of free spinless fermions and consider random diagonal disorder. In the instantaneous basis, we compute the polarization, the entanglement spectrum, and the local Chern marker. As a first main result, we conclude that the space-integrated local Chern marker is best suited for a quantitative determination of topological transitions in a disordered system. In the time-dependent simulations, we use the time-integrated current to obtain the pumped charge in slowly periodically driven systems. As a second main result, we observe and characterize a disorder-driven breakdown of the quantized charge pump. There is an excellent agreement between the static and the time-dependent ways of computing the pumped charge. The topological transition occurs well in the regime where all states are localized on the given system sizes and is therefore not tied to a delocalization-localization transition of Hamiltonian eigenstates. For individual disorder realizations, the breakdown of the quantized pumping occurs for parameters where the spectral bulk gap inherited from the band gap of the clean system closes, leading to a globally gapless spectrum. As a third main result and with respect to the analysis of finite-size systems, we show that the disorder average of the bulk gap severely overestimates the stability of quantized pumping. A much better estimate is the typical value of the distribution of energy gaps, also called mode of the distribution.