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基于精确电子-核动力学的分子几何相的出现

Emergence of the Molecular Geometric Phase from Exact Electron-Nuclear Dynamics.

作者信息

Martinazzo Rocco, Burghardt Irene

机构信息

Department of Chemistry, Università degli Studi di Milano, Via Golgi 19, 20133 Milano, Italy.

Institute of Physical and Theoretical Chemistry, Goethe University Frankfurt, Max-von-Laue-Str. 7, D-60438 Frankfurt/Main, Germany.

出版信息

J Phys Chem Lett. 2024 Oct 17;15(41):10416-10424. doi: 10.1021/acs.jpclett.4c02035. Epub 2024 Oct 10.

Abstract

Geometric phases play a crucial role in diverse fields. In molecules, they appear when a reaction path encircles an intersection between adiabatic potential energy surfaces and the molecular wave function experiences quantum-mechanical interference effects. This intriguing effect, closely resembling the magnetic Aharonov-Bohm effect, crucially relies on the adiabatic description of the dynamics, and it is an open issue whether and how it persists in an exact quantum dynamical framework. Recent works suggest that the molecular geometric phase is an artifact of the adiabatic approximation, thereby challenging the entire concept. Here, building upon a recent investigation (Martinazzo, R.; Burghardt, I. , , 243002), we address this issue using the exact factorization of the total wave function. We introduce instantaneous gauge-invariant phases separately for the electrons and nuclei and use them to monitor the phase difference between the trailing edges of a wavepacket encircling a conical intersection between adiabatic surfaces. The transition from the time-dependent open-path phase differences to the closed-path limit is examined, revealing how the phase differences in the electronic and nuclear subspaces compensate for each other upon path closure. In this way, we unambiguously demonstrate the role of the geometric phase in the interference process and shed light on its persistence beyond the adiabatic approximation.

摘要

几何相位在多个领域中都起着至关重要的作用。在分子中,当反应路径环绕绝热势能面之间的交叉点时,几何相位就会出现,分子波函数会经历量子力学干涉效应。这种有趣的效应与磁阿哈罗诺夫 - 玻姆效应极为相似,它关键依赖于动力学的绝热描述,而在精确的量子动力学框架中它是否存在以及如何存在仍是一个悬而未决的问题。近期的研究表明分子几何相位是绝热近似的产物,从而对整个概念提出了挑战。在此,基于最近的一项研究(Martinazzo, R.; Burghardt, I.,,, 243002),我们使用总波函数的精确因式分解来解决这个问题。我们分别为电子和原子核引入瞬时规范不变相位,并利用它们来监测围绕绝热面之间锥形交叉点的波包后沿之间的相位差。研究了从与时间相关的开放路径相位差到封闭路径极限的转变,揭示了电子和原子核子空间中的相位差在路径封闭时如何相互补偿。通过这种方式,我们明确地证明了几何相位在干涉过程中的作用,并阐明了它在绝热近似之外的持续性。

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