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用于空间非均匀非厄米系统的相空间广义布里渊区

Phase-Space Generalized Brillouin Zone For Spatially Inhomogeneous Non-Hermitian Systems.

作者信息

Li Qingya, Jiang Hui, Lee Ching Hua

机构信息

Department of Physics, National University of Singapore, Singapore, 117551, Singapore.

School of Physics, Dalian University of Technology, Dalian, 116024, China.

出版信息

Adv Sci (Weinh). 2025 Aug 11:e08047. doi: 10.1002/advs.202508047.

Abstract

The generalized Brillouin zone (GBZ) is highly successful in characterizing the topology and band structure of non-Hermitian systems. However, its applicability ischallenged in spatially inhomogeneous settings, where the non-locality of non-Hermitian pumping competes with Wannier-Stark localization and quantum interference, potentially leading to highly non-exponential state accumulation. To transcend this major conceptual bottleneck, a general phase-space GBZ formalism is developed that encodes non-Bloch deformations in both position and momentum space, such as to accurately represent spatially inhomogeneous non-Hermitian pumping. A key new phenomenon is the bifurcation of the phase-space GBZ branches, which allows certain eigenstates to jump abruptly between different GBZ solutions at various points in real space, such as to accommodate pockets of inhomogeneity. The freedom in the jump locations opens up an emergent degree of freedom that protects the stability of real spectra and, more impressively, the robustness of a new class of topological zero modes unique to GBZ bifurcation. The response from these novel spectral and GBZ singularities can be readily demonstrated in mature metamaterial platforms such as photonic crystals or circuit arrays. The framework directly generalizes to more complicated unit cells and further hoppings, opening up a vast new arena for exploring unconventional spectral and topological transitions, as well as GBZ fragmentation in spatially inhomogeneous non-Hermitian settings.

摘要

广义布里渊区(GBZ)在表征非厄米系统的拓扑结构和能带结构方面非常成功。然而,在空间非均匀的情况下,其适用性受到挑战,在这种情况下,非厄米泵浦的非局域性与万尼尔 - 斯塔克局域化和量子干涉相互竞争,可能导致高度非指数形式的态积累。为了突破这一主要概念瓶颈,开发了一种通用的相空间GBZ形式主义,它在位置和动量空间中编码非布洛赫变形,以便准确地表示空间非均匀的非厄米泵浦。一个关键的新现象是相空间GBZ分支的分岔,这使得某些本征态能够在实空间的不同点在不同的GBZ解之间突然跳跃,从而适应不均匀性区域。跳跃位置的自由度开辟了一种新出现的自由度,它保护实谱的稳定性,更令人印象深刻的是,保护一类独特的GBZ分岔拓扑零模的鲁棒性。这些新颖的谱和GBZ奇点的响应可以在成熟的超材料平台(如光子晶体或电路阵列)中很容易地得到证明。该框架直接推广到更复杂的晶胞和进一步的跳跃,为探索非常规的谱和拓扑转变以及空间非均匀非厄米环境中的GBZ碎片化开辟了一个广阔的新领域。

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