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第二周期四原子团簇X4(X = Na、Mg、Al、Si、P、S)中几何结构和赝旋转的赝 Jahn-Teller 起源

Pseudo-Jahn-Teller origin of geometry and pseudorotations in second row tetra-atomic clusters X4 (X=Na, Mg, Al, Si, P, S).

作者信息

Garcia-Fernandez Pablo, Bersuker Isaac B, Boggs James E

机构信息

Institute for Theoretical Chemistry, The University of Texas at Austin, Chemistry and Biochemistry Department, Austin, Texas 78712-0165, USA.

出版信息

J Chem Phys. 2006 Jan 28;124(4):044321. doi: 10.1063/1.2150436.

Abstract

Experimentally determined or ab initio calculated molecular geometries carry no information about their origin. Employing the Jahn-Teller (JT) vibronic coupling effects as the only source of instability and consequent distortions of high-symmetry molecular configurations, we have worked out a procedure that allows us to trace the origin of particular geometries and determine the detailed electronic mechanism of their formation. This procedure is illustrated by considering a series of X(4) clusters with X=Na, Mg, Al, Si, P, and S. It shows explicitly why Na(4), Si(4), and Al(4) have a rhombic geometry in the ground state, while Mg(4) and P(4) are tetrahedral, whereas S(4) is a trapezium. Even when the minimum-energy geometries are the same (as in the case of rhombic Na(4), Si(4), and Al(4)), the electronic mechanism of their formation is quite different. In particular, in Na(4) and Si(4) the rhombic minima are produced by a strong pseudo JT coupling between two excited states in the square-planar configuration (different in the two cases) that stabilizes one of them and makes it the ground state by rhombic distortions. The rhombic configuration of Al(4) is due to the pseudo JT effect in its ground-state square-planar configuration, and the trapezium in S(4) is formed by two pseudo JT couplings essentially involving excited states. In several cases this analysis shows also the tunneling paths between equivalent configurations.

摘要

实验测定或从头计算得到的分子几何结构并未携带有关其起源的信息。我们将 Jahn-Teller(JT)电子振动耦合效应作为高对称分子构型不稳定性及随之产生畸变的唯一来源,制定了一种方法,该方法能让我们追溯特定几何结构的起源,并确定其形成的详细电子机制。通过考虑一系列 X(4) 簇(其中 X = Na、Mg、Al、Si、P 和 S)来说明这一方法。它明确展示了为什么 Na(4)、Si(4) 和 Al(4) 在基态具有菱形几何结构,而 Mg(4) 和 P(4) 是四面体结构,而 S(4) 是梯形结构。即使最低能量几何结构相同(如菱形的 Na(4)、Si(4) 和 Al(4) 的情况),它们形成的电子机制也大不相同。特别是,在 Na(4) 和 Si(4) 中,菱形极小值是由平面正方形构型中两个激发态之间的强赝 JT 耦合产生的(两种情况不同),这种耦合使其中一个激发态稳定,并通过菱形畸变使其成为基态。Al(4) 的菱形构型归因于其基态平面正方形构型中的赝 JT 效应,而 S(4) 中的梯形是由两个基本上涉及激发态的赝 JT 耦合形成的。在几种情况下,这种分析还显示了等效构型之间的隧穿路径。

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