A semiclassical model for tunneling from one classically allowed region on a potential energy surface to another is described. The principal feature of this model, compared to earlier (more ‘‘rigorous’’) multidimensional semiclassical tunneling theories, is that it can be implemented in a straightforward way within the framework of a standard classical trajectory simulation. Applications to several examples of unimolecular isomerization and unimolecular dissociation show that the model is capable of providing excellent results over a wide range of conditions (i.e., coupling strengths, different symmetries of couplings, etc.)

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Equation (2.2a) is correct for small tunneling probabilities, Pn≪1. More generally, one must include a “survival probability” factor, so that Eq. (2.2a)becomes Pnet(t) = Σn = 1h(t−tn)pn, where p1 = P1 and pn = Pn(1−Σn = 1n−1Pn) for n>1, with Pn still given by Eq. (2.2b).
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