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Minimum energy coordinates electronic-nuclear interaction

The import of diabatic electronic states for dynamical treatments of conical intersecting BO potential energy surfaces is well acknowledged. This intersection is characterized by the non-existence of symmetry element determining its location in nuclear space [25]. This problem is absent in the GED approach. Because the symmetries of the cis and trans conformer are irreducible to each other, a regularization method without a correct reaction coordinate does not make sense. The slope at the (conic) intersection is well defined in the GED scheme. Observe, however, that for closed shell structures, the direct coupling of both states is zero. A configuration interaction is necessary to obtain an appropriate description in other words, correlation states such as diradical ones and the full excited BB state in the AA local minimum cannot be left out the scheme. [Pg.192]


See other pages where Minimum energy coordinates electronic-nuclear interaction is mentioned: [Pg.5]    [Pg.157]    [Pg.108]    [Pg.344]    [Pg.261]    [Pg.611]    [Pg.357]    [Pg.16]    [Pg.110]    [Pg.131]    [Pg.111]    [Pg.611]    [Pg.43]    [Pg.17]    [Pg.100]    [Pg.149]    [Pg.21]   
See also in sourсe #XX -- [ Pg.474 ]




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1 energy minimum

Coordinates electron

Coordination interaction

Electronic coordinate

Electronic energy minimum

Electronic interactions

Energy electronic interaction

Interaction coordinate

Interaction electron-nuclear

Interaction energy

Nuclear coordinate

Nuclear energy

Nuclear interaction

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