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.