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arXiv 2202.07684cond-mat.mes-hallcond-mat.mtrl-scicond-mat.quant-gascond-mat.str-elquant-ph
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玻色格林函数的边界相关动力学不稳定性:耗散Bogoliubov-de Gennes哈密顿量及其在非厄米趋肤效应中的应用

Boundary-dependent dynamical instability of bosonic Green's function: Dissipative Bogoliubov-de Gennes Hamiltonian and its application to non-Hermitian skin effect

Nobuyuki Okuma

摘要:

凝聚体的玻色子激发能谱由非厄米哈密顿量的谱给出,该非厄米哈密顿量一般由玻色子Bogoliubov-de Gennes(BdG)哈密顿量构造,即使该系统本质上是厄米哈密顿量。换句话说,两种类型的非厄米性可以共存:一种来自玻色子BdG性质,另一种来自开放量子性质。在本文中,我们提出了边界相关的动力学不稳定性。本文首先在Nambu空间中用格林函数定义了玻色耗散BdG哈密顿量,并讨论了相应的非厄米哈密顿量的正确的粒子-空穴对称性。然后,我们构建了一个模型的边界相关的动力学不稳定性,使它满足正确的粒子-空穴对称性。在这个模型中,打破粒子数守恒的反常项表示BdG性质的非厄米性,而正常项由耗散的Hatano-Nelson模型给出。由于两种非厄米性之间的竞争,光谱的虚部可以是正的,而不需要正常部分的放大和导致朗道不稳定性的粒子-空穴带接触的帮助。这导致了边界相关的动力学不稳定性下的非厄米集肤效应,-强依赖性的光谱边界条件的非厄米哈密顿-,的Bogoliubov谱。

英文摘要:

The energy spectrum of bosonic excitations from a condensate is given by the spectrum of a non-Hermitian Hamiltonian constructed from a bosonic Bogoliubov-de Gennes (BdG) Hamiltonian in general even though the system is essentially Hermitian. In other words, two types of non-Hermiticity can coexist: one from the bosonic BdG nature and the other from the open quantum nature. In this paper, we propose boundary-dependent dynamical instability. We first define the bosonic dissipative BdG Hamiltonian in terms of Green's function in Nambu space and discuss the correct particle-hole symmetry of the corresponding non-Hermitian Hamiltonian. We then construct a model of the boundary-dependent dynamical instability so that it satisfies the correct particle-hole symmetry. In this model, an anomalous term that breaks the particle number conservation represents the non-Hermiticity of the BdG nature, while a normal term is given by a dissipative Hatano-Nelson model. Thanks to the competition between the two types of non-Hermiticity, the imaginary part of the spectrum can be positive without the help of the amplification of the normal part and the particle-hole band touching that causes the Landau instability. This leads to the boundary-dependent dynamical instability under the non-Hermitian skin effect, -strong dependence of spectra on boundary conditions for non-Hermitian Hamiltonians-, of the Bogoliubov spectrum.

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