Vibrational Transitions
The second term in the
expansion of the dipole moment as a function of nuclear coordinate

gives rise to the vibrational
transitions.
The vibrational
wave functions

form an orthonormal set of wave
functions, cn. The first few vibrational
wave functions are listed below.

The orthonormality
can be illustrated using the first two wave functions in the set:

The last integral is an odd
function over even limits. If we now
consider the second term in the dipole expansion as a
operator we have:

Thus, the vibrational
transition moment for the transition from v = 0 to v = 1 is:

Vibrational selection rules arise from the fact that the integral
for transition from v = 0 to v > 1 is zero.
For example,

Both of the integrals are odd functions over even
limits. While we do not prove the
general expression here it can be shown that transitions occur from v à v’ where v’ = v ±
1.
This is depicted below.
