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通过混合量子-经典刘维尔方法研究溶解在极性液体中的氢键复合物的振动能量弛豫。

Vibrational energy relaxation of a hydrogen-bonded complex dissolved in a polar liquid via the mixed quantum-classical Liouville method.

作者信息

Hanna Gabriel, Geva Eitan

机构信息

Department of Chemistry and FOCUS center, University of Michigan, Ann Arbor, Michigan 48109-1055, USA.

出版信息

J Phys Chem B. 2008 Apr 3;112(13):4048-58. doi: 10.1021/jp076155b. Epub 2008 Mar 11.

Abstract

The vibrational energy relaxation (VER) of the hydrogen stretch in a linear hydrogen-bonded complex dissolved in a polar solvent is studied. The study is based on the Azzouz-Borgis model [Azzouz, H.; Borgis, D. J. Chem. Phys. 1993, 98, 7361], which is known to account for many important features of real hydrogen-bonded systems, including ionic-to-covalent tautomerism and a broad distribution of hydrogen stretch frequencies. A description of VER in this strongly coupled system is considered, which consists of the following three consecutive steps: (1) solvation on the adiabatic excited vibrational surface; (2) nonadiabatic transition from the excited to the ground adiabatic vibrational surface; and (3) solvation on the adiabatic ground vibrational surface. The relaxation dynamics during those three steps were simulated via the mixed quantum-classical Liouville method, where the hydrogen is treated quantum-mechanically, while the other particles are treated in a classical-like manner. The solvation on the excited-state surface was found to occur rapidly ( approximately 0.5 ps) and to involve energy exchange with both the intramolecular and intermolecular degrees of freedom. It was also found that, while energy is released to the solvent during the solvation of the covalent tautomer, the solvation of the ionic tautomer involves absorption of energy from the solvent. The decrease in the transition frequency during the solvation process also facilitates the nonadiabatic transitions, which occur rapidly ( approximately 0.8 ps) thereafter. The nonadiabatic transitions were shown to be induced by interactions with a large number of solvent molecules and to be relatively insensitive to their location relative to the complex. Finally, solvation on the ground-state surface was seen to occur on a time scale of approximately 1.0 ps and leads to nonequilibrium ionic and covalent subpopulations. Equilibration on the ground-state surface occurs on a significantly slower time scale ( approximately 7.6 ps). Our results shed new light on the problem of VER in strongly coupled condensed phase systems that lie outside the range of validity of the Landau-Teller formula.

摘要

研究了溶解在极性溶剂中的线性氢键复合物中氢伸缩振动的能量弛豫(VER)。该研究基于阿祖兹 - 博尔吉斯模型[Azzouz, H.; Borgis, D. J. Chem. Phys. 1993, 98, 7361],已知该模型能够解释真实氢键系统的许多重要特征,包括离子 - 共价互变异构以及氢伸缩频率的广泛分布。本文考虑了对这个强耦合系统中VER的描述,它由以下三个连续步骤组成:(1)在绝热激发振动表面上的溶剂化;(2)从激发绝热振动表面到基态绝热振动表面的非绝热跃迁;(3)在绝热基态振动表面上的溶剂化。通过混合量子 - 经典刘维尔方法模拟了这三个步骤中的弛豫动力学,其中氢采用量子力学处理,而其他粒子采用类似经典的方式处理。发现激发态表面上的溶剂化迅速发生(约0.5皮秒),并且涉及与分子内和分子间自由度的能量交换。还发现,虽然在共价互变异构体的溶剂化过程中能量释放到溶剂中,但离子互变异构体的溶剂化涉及从溶剂中吸收能量。溶剂化过程中跃迁频率的降低也促进了非绝热跃迁,此后非绝热跃迁迅速发生(约0.8皮秒)。非绝热跃迁被证明是由与大量溶剂分子的相互作用引起的,并且对它们相对于复合物的位置相对不敏感。最后,基态表面上的溶剂化发生在约1.0皮秒的时间尺度上,并导致非平衡的离子和共价亚群。基态表面上的平衡在明显更慢的时间尺度(约7.6皮秒)上发生。我们的结果为兰道 - 泰勒公式有效性范围之外的强耦合凝聚相系统中的VER问题提供了新的见解。

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