Abstract

Semiclassical versions of the static (diabatic) and adiabatic coupling schemes are applied to a two-level-one-mode system at total energies above the cross-over level. The corresponding rates of nonradiative multiphonon transitions reduce to alternativemonotonous dependences on the usual Landau-Zener parameterγ. Static coupling gives an increasing transition probability (per oscillation) of the familiar formPst(γ) = 4πγ. Adiabatic coupling associated with a sufficiently low mechanism-specific potential barrier of Born's type produces a decreasing transition probability of the formPad(γ) exp (−2πγ). The underlying “Beyond-Non-Condon” calculation procedure shows that (1) the weak dependence of the pre-exponential factorPad is a consequence of theγ-independent normalization of the electronic matrix element governing the non-adiabaticity operator and (2) the occurrence of the mechanism-specific tunnelling factor exp(−2πγ) is due to the avoided crossing of adiabatic oscillator potentials. Ranges of applicability of both alternative coupling schemes are limited by comparison with earlier non-perturbational results.

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