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Vibration-rotation Hamiltonians angles

Given the bend state or angle dependent Hamiltonian, one may easily generalise the collinear TST, with harmonic tunneling correction to 3D systems. The rotationally averaged cross section from initial vibrational state n summed over all final vibrational (n ) and rotational (j ) states is defined as ... [Pg.158]

See other pages where Vibration-rotation Hamiltonians angles is mentioned: [Pg.612]    [Pg.181]    [Pg.505]    [Pg.59]    [Pg.613]    [Pg.304]    [Pg.317]    [Pg.181]    [Pg.613]    [Pg.349]    [Pg.181]    [Pg.498]    [Pg.144]    [Pg.63]    [Pg.509]    [Pg.511]    [Pg.337]    [Pg.167]    [Pg.617]    [Pg.619]    [Pg.201]    [Pg.201]    [Pg.83]    [Pg.8]    [Pg.335]    [Pg.196]    [Pg.368]    [Pg.295]    [Pg.3]    [Pg.59]    [Pg.144]    [Pg.155]    [Pg.167]    [Pg.617]    [Pg.619]    [Pg.201]    [Pg.91]    [Pg.8]    [Pg.155]    [Pg.42]    [Pg.85]    [Pg.218]    [Pg.340]    [Pg.347]    [Pg.156]    [Pg.154]    [Pg.530]   
See also in sourсe #XX -- [ Pg.332 , Pg.333 ]



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