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Photoselective chemistry access to the transition state region

Photoselective chemistry access to the transition state region [Pg.264]

As the wavelength of lasers gets shorter and shorter we can also envisage approaching the limit where the light will be used in a diffraction mode, simitar to the current uses of X-rays. Combined with ultrashort pulses, Chapter 8, this will allowtcacldng the structure of molecules during chemical, biochemical, and material (e.g., fracture) processes. [Pg.264]

The quantum analog of the classical Franck-Condon principle is that the probability of the nuclei making a transition from one potential surface to another is [Pg.265]

for identical potential curves in the ground and excited states, the vibrational selection rule Av = 0 is strictly obeyed for whatever vibrational level v in which the nuclei start. We refer to such a limiting situation as having diagonal Franck-Condon factors. [Pg.267]

Suppose that the two potential surfaces are dissimilar. Then the Franck-Condon factors are less than imity and you get different probabilities for making transitions to final v vibrational levels depending on the vibrational overlap. We shall make repeated use of the Franck-Condon principle in imderstanding which vibrational levels are populated in various dynamical processes. In Section 9.2 we will generalize the principle so that it also applies to excitation as a result of a collision (where we need not be in the sudden limit). [Pg.267]




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Access to Chemistry

Photoselection

Photoselective chemistry

The Region

The Transition State

The transition region

Transition chemistry

Transition region

Transition state region

Transitional regions

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