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首页> 外文期刊>The Journal of Chemical Physics >On the adiabatic to diabatic states transformation in the presence of a conical intersection: A most diabatic basis from the solution to a Poisson's equation. I
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On the adiabatic to diabatic states transformation in the presence of a conical intersection: A most diabatic basis from the solution to a Poisson's equation. I

机译:关于在圆锥形相交处的绝热状态到绝热状态的转换:从解到泊松方程的最绝热基础。一世

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We report the first determination of "most" diabatic basis for a triatomic molecule based exclusively on ab initio derivative couplings that takes careful account of the limitations imposed by the nonremovable part of those couplings. Baer [Chem. Phys. Lett. 35, 112 (1975)] showed that an orthogonal transformation from adiabatic states to diabatic states cannot remove all the derivative coupling unless the curl of the derivative coupling vanishes. Subsequently, Mead and Truhlar [J. Chem. Phys. 77, 6090 (1982)] observed that this curl does not, in general, vanish so that some of the derivative coupling is nonremovable. This observation and the historical lack of efficient algorithms for the evaluation of the derivative coupling led to a variety of methods for determining approximate diabatic bases that avoid computation of the derivative couplings. These methods neglect an indeterminate portion of the derivative coupling. Mead and Truhlar also observed that near an avoided crossing of two stales the rotation angle to a most diabatic basis, i.e., the basis in which the removable part of the derivative coupling has been transformed away, could be obtained from the solution of a Poisson's equation requiring only knowledge of the derivative couplings. Here a generalization of this result to the case of a conical intersection is used to determine a most diabatic basis for a section of the 1 (1)A' and 2( 1)A' potential energy surfaces of HeH2 that includes the minimum energy point on the seam of conical intersection. (C) 1998 American Institute of Physics. [S0021-9606(98)01725-5]. [References: 37]
机译:我们报告的三原子分子的“最”绝热基础的第一个确定完全基于从头算起的派生耦合,其中仔细考虑了那些耦合的不可移动部分所施加的限制。贝尔[Chem。物理来吧35,112(1975)]表明,从绝热态到非绝热态的正交变换不能消除所有的导数耦合,除非导数耦合的卷曲消失。随后,米德和特鲁拉尔[J.化学物理77,6090(1982)]观察到,这种卷曲通常不会消失,因此某些导数耦合是不可移动的。这种观察和历史上缺乏用于评估导数耦合的有效算法的方法导致了用于确定避免计算导数耦合的近似绝热基数的多种方法。这些方法忽略了微分耦合的不确定部分。 Mead和Truhlar还观察到,在避免避开两个变角的交点附近,旋转角至最绝热的基础,即微分耦合的可移动部分已被变换掉的基础,可以从泊松方程的解中获得。只需要微分耦合的知识。在此,将结果推广到圆锥形相交的情况下,用于确定HeH2的1(1)A'和2(1)A'势能面的截面的最绝热基础,该截面包括最小能量点在圆锥形相交处。 (C)1998美国物理研究所。 [S0021-9606(98)01725-5]。 [参考:37]

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