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Band Shape The Huang-Rhys Coupling Parameter

5 BAND SHAPE THE HUANG-RHYS COUPLING PARAMETER [Pg.175]

The overall absorption probabihty at 0 K involves a summation of the probabilities from the ground vibrational state, = 0, to all of the excited m states (m = 0, 1, 2.), and so it can be written as follows  [Pg.176]

The absorption (emission) band shape at 0 K can be estimated from Equation (5.30) if the square of the overlap integral of harmonic functions, l(Xm(2)l/o(2) P. is known for each excited (terminal) m level. Using the wavefunctions of the harmonic oscillator, these overlap functions can be expressed as a function of S  [Pg.177]

we can predict the relative intensity of each 0 m absorption line using this expression together with Equation (5.30)  [Pg.177]

We must recall that that, according to Equation (5.31), the full absorption intensity (the area under the absorption band) is independent of S. Thus, the factor e (which corresponds to /o o) represents the fraction of the absorption intensity taken by the zero-phonon line, while the intensity /o i = e x S represents the fractional intensity related to the 0 1 transition, Iq 2 = x (5 /2) the fractional intensity of the 0 2 transition, and so on. [Pg.177]




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Coupling parameter

Huang-Rhys parameter

The Bands

The parameters

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