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从头算腔量子电动力学中相干态变换的微扰分析。

Perturbative analysis of the coherent state transformation in ab initio cavity quantum electrodynamics.

作者信息

Roden Peyton, Foley Jonathan J

机构信息

Department of Chemistry, University of North Carolina Charlotte, 9201 University City Boulevard, Charlotte, North Carolina 28223, USA.

出版信息

J Chem Phys. 2024 Nov 21;161(19). doi: 10.1063/5.0233717.

Abstract

Experimental demonstrations of modified chemical structure and reactivity under strong light-matter coupling have spurred theoretical and computational efforts to uncover underlying mechanisms. Ab initio cavity quantum electrodynamics (QED) combines quantum chemistry with cavity QED to investigate these phenomena in detail. Unitary transformations of ab initio cavity QED Hamiltonians have been used to make them more computationally tractable. We analyze one such transformation, the coherent state transformation, using perturbation theory. Applying perturbation theory up to third order for ground state energies and potential energy surfaces of several molecular systems under electronic strong coupling, we show that the coherent state transformation yields better agreement with exact ground state energies. We examine one specific case using perturbation theory up to ninth order and find that coherent state transformation performs better up to fifth order but converges more slowly to the exact ground state energy at higher orders. In addition, we apply perturbation theory up to second order for cavity mode states under bilinear coupling, elucidating how the coherent state transformation accelerates the convergence of the photonic subspace toward the complete basis limit and renders molecular ion energies origin invariant. These findings contribute valuable insights into computational advantages of the coherent state transformation in the context of ab initio cavity quantum electrodynamics methods.

摘要

在强光 - 物质耦合下,化学结构和反应性的改变的实验证明激发了理论和计算方面的努力,以揭示其潜在机制。从头算腔量子电动力学(QED)将量子化学与腔QED相结合,以详细研究这些现象。从头算腔QED哈密顿量的酉变换已被用于使其在计算上更易于处理。我们使用微扰理论分析一种这样的变换,即相干态变换。对于电子强耦合下的几个分子系统的基态能量和势能面,应用高达三阶的微扰理论,我们表明相干态变换与精确基态能量具有更好的一致性。我们使用高达九阶的微扰理论研究一个特定情况,发现相干态变换在五阶之前表现更好,但在高阶时向精确基态能量的收敛更慢。此外,对于双线性耦合下的腔模态,我们应用高达二阶的微扰理论,阐明了相干态变换如何加速光子子空间向完全基极限的收敛,并使分子离子能量原点不变。这些发现为从头算腔量子电动力学方法中相干态变换的计算优势提供了有价值的见解。

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