Jahn-Teller selection rules

A-jg) transition which is symmetry and parity allowed for an electric dipole transition mechanism the spin selection rule is suspended by the large spin orbit coupling of about Ijp 3T 2 400 cm (j 2). Since analysis of the progressions yields, for both compounds, only eg quanta (240 cm 1 for Cl, 154cm 1 for Br) the excitea state must be distorted by Jahn-Teller forces... 

Simple examples of these effects were discussed in Section IV as limiting cases of the pseudo-Jahn Teller and pseudo-Renner-Teller effects. There it was shown that instead of using the adiabatic approximation, we should, in the interest of convenience, adopt a diabatic approximation in which the electronic degeneracy is maintained in zeroth order. The splitting can then simply be ascribed to adiabatic coupling proportional to Q, (or Qf, etc.) or to Qf (or Qf, etc.) between the two electronic components that remain degenerate at Q, = 0. The selection rule for pseudo-Jahn Teller coupling is thus <0° 0 or, iff denotes representation, T , x F,- x F 3-4,. 

The presumably most widely known example of vibronic coupling is the Jahn-Teller effect of a doubly degenerate electronic state, that is, the coupling of the two components of the degenerate state by a doubly degenerate vibrational mode. The symmetry selection rule for this type of vibronic coupling, the so-called E x E Jahn-Teller effect, is °... 

The general principles for the construction of the vibronic Hamiltonian and the symmetry selection rules are the same as indicated above and discussed in more detail in Chapter 7. The previous distinction between trigonal and tetragonal point groups does not play a role, and the first-order coupling is always accomplished by doubly degenerate (e) vibrational modes. In an analogous notation as in Eq. (3), the Hamiltonian for the linear (E + A) (g) e pseudo-Jahn-Teller effect is found to... 

---