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arXiv 1507.04726cond-mat.mes-hall
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电子-声子相互作用的多体格林函数理论:Holstein二聚体光谱性质的Kadanoff-Baym方法

Many-body Green's function theory for electron-phonon interactions: the Kadanoff-Baym approach to spectral properties of the Holstein dimer

N. Säkkinen, Y. Peng, H. Appel, R. van Leeuwen

摘要:

在多体微扰理论框架下,我们提出了一种研究电子与声子相互作用系统的含时现象的Kadanoff-Baym形式。的形式主义正确地考虑到平衡态的初始准备的影响,并允许一个明确的时间依赖性的电子和声子的自由度。应用该方法研究了均匀双位双电子Holstein模型的电荷中性和非中性激发谱。这是文献[arXiv:1403.2968]中发表的Hartree(H)、部分自洽Born(Gd)和完全自洽Born(GD)近似中基态性质的先前研究的扩展。我们表明,选择一个均匀的基态解决方案,导致不稳定的动力学足够的强相互作用,并允许一个连续破碎的状态,防止这一点。这种不稳定性是由基态的分叉引起的,物理上理解为与精确系统的双极化交叉有关。这种平均场不稳定性在部分自洽玻恩近似中仍然存在,但在完全自洽玻恩近似中没有发现。通过理解稳定性,我们能够通过计算时间传播的密度-密度响应函数来研究线性响应区域。该函数相当于具有复杂内核的Bethe-Salpeter方程的解。结果表明,没有一个近似是能够描述的响应函数期间或之后的双极化交叉的参数调查。总的来说,我们提供了一个广泛的讨论时,近似是有效的,以及它们如何无法描述所选择的模型系统的研究的确切属性。

英文摘要:

We present a Kadanoff-Baym formalism to study time-dependent phenomena for systems of interacting electrons and phonons in the framework of many-body perturbation theory. The formalism takes correctly into account effects of the initial preparation of an equilibrium state, and allows for an explicit time-dependence of both the electronic and phononic degrees of freedom. The method is applied to investigate the charge neutral and non-neutral excitation spectra of a homogeneous, two-site, two-electron Holstein model. This is an extension of a previous study of the ground state properties in the Hartree (H), partially self-consistent Born (Gd) and fully self-consistent Born (GD) approximations published in Ref. [arXiv:1403.2968]. We show that choosing a homogeneous ground state solution leads to unstable dynamics for a sufficiently strong interaction, and that allowing a symmetry-broken state prevents this. The instability is caused by the bifurcation of the ground state and understood physically to be connected with the bipolaronic crossover of the exact system. This mean-field instability persists in the partially self-consistent Born approximation but is not found for the fully self-consistent Born approximation. By understanding the stability properties, we are able to study the linear response regime by calculating the density-density response function by time-propagation. This functions amounts to a solution of the Bethe-Salpeter equation with a sophisticated kernel. The results indicate that none of the approximations is able to describe the response function during or beyond the bipolaronic crossover for the parameters investigated. Overall, we provide an extensive discussion on when the approximations are valid, and how they fail to describe the studied exact properties of the chosen model system.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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