Anomalous pumping in the non-Hermitian Rice-Mele model.

IF 2.3 4区 物理与天体物理 Q3 PHYSICS, CONDENSED MATTER Journal of Physics: Condensed Matter Pub Date : 2025-02-04 DOI:10.1088/1361-648X/ada982
Abhishek Kumar, Sarbajit Mazumdar, S D Mahanti, Kush Saha
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Abstract

We study topological charge pumping in the Rice-Mele (RM) model with irreciprocal hopping. The non-Hermiticity gives rise to interesting pumping physics, owing to the presence of skin effect and exceptional points. In the static one-dimensional (1D) RM model, we find two independent tuning knobs that can drive the topological transition, namely, non-Hermitian parameterγand system sizeN. To elucidate the system-size dependency, we use a finite-size generalized Brillouin zone scheme to show that the edge modes can be distinguished from the non-hermiticity induced skin modes. Moreover, this scheme can capture the state pumping of topological edge modes as a function ofγin the static 1D RM model and it further provides insight into engineering novel gapless exceptional edge modes with the help of adiabatic drive. Furthermore, we show that the standard topological pumping due to the adiabatic and periodic variation of the model parameters survives even with finiteγ. However, we observe that it depends upon the driving protocols and strength of the non-Hermiticity (γ). With increasingγ, the adiabatic pumping for non-trivial protocols is destroyed first and then re-emerges as an anomalous pumping which does not have any Hermitian counterpart. Additionally, we observe that even a trivial adiabatic protocol can give rise to pumping as opposed to the Hermitian system. This is attributed to the inherent point gap physics of non-Hermitian system which we explain by reformulating a non-Bloch topological invariant for the 1+1D RM model. This invariant explains the number of pumped charges (in each period) for all the driving protocols.

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非厄米Rice-Mele模型中的异常抽运。
研究了具有不互反跳变的Rice-Mele (RM)模型中的拓扑电荷抽运(TCP)问题。由于趋肤效应和特殊点的存在,非厄米性产生了有趣的抽运物理。在静态一维(1D) RM模型中,我们找到了两个独立的调谐旋涡来驱动拓扑转换,即非厄米参数$\gamma$和系统大小$N$。为了阐明系统大小的依赖性,我们使用有限大小的广义布里温区(GBZ)格式来证明边缘模式可以与非厄米性诱导的表皮模式区分开来。此外,该方案可以捕获拓扑边缘模式的状态泵送作为静态1D RM模型中$\gamma$的函数,并进一步提供了借助绝热驱动的工程新型无间隙异常边缘模式的见解。此外,我们证明了由于模型参数的绝热和周期性变化而导致的标准拓扑泵浦即使在有限的$\gamma$下仍然存在。然而,我们观察到它取决于驱动协议和非厄米性($\gamma$)的强度。随着$\gamma$的增大,非平凡协议的绝热抽运首先被破坏,然后以不存在厄米对偶的异常抽运重新出现。此外,我们观察到,即使是一个微不足道的绝热协议也可以产生与厄米系统相反的抽运。这归因于非厄米系统固有的点间隙物理,我们通过重新表述1+1D RM模型的非bloch拓扑不变量来解释这一点。这个不变量解释了所有驱动协议的抽运电荷(在每个周期)的数量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Journal of Physics: Condensed Matter
Journal of Physics: Condensed Matter 物理-物理:凝聚态物理
CiteScore
5.30
自引率
7.40%
发文量
1288
审稿时长
2.1 months
期刊介绍: Journal of Physics: Condensed Matter covers the whole of condensed matter physics including soft condensed matter and nanostructures. Papers may report experimental, theoretical and simulation studies. Note that papers must contain fundamental condensed matter science: papers reporting methods of materials preparation or properties of materials without novel condensed matter content will not be accepted.
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