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Anharmonic coupling theory Hamiltonian modes

As a consequence of the above equations, the full Hamiltonian describing the fast mode coupled to the H-bond bridge (via the strong anharmonic coupling theory) and to the bending mode (via the Fermi resonance process) may be written within the tensorial basis (222) according to [24] ... [Pg.324]

Several studies of Fermi resonances in the absence of H bond have been made [76-80]. We shall account for this situation by simply ignoring the anharmonic coupling between the fast and slow modes (a = 0). The theory then describes the coupling between the fast mode and a bending mode through the potential Htf, with both of these modes being damped in the same way. Because aG = 0, the slow mode does not play any role, so that the total Hamiltonian does not refer to it ... [Pg.275]


See other pages where Anharmonic coupling theory Hamiltonian modes is mentioned: [Pg.251]    [Pg.256]    [Pg.210]    [Pg.260]    [Pg.4]    [Pg.445]    [Pg.309]    [Pg.340]    [Pg.265]    [Pg.168]    [Pg.171]    [Pg.324]    [Pg.14]    [Pg.3157]    [Pg.800]   
See also in sourсe #XX -- [ Pg.256 , Pg.257 ]




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