(a) Let (x, y, z) denote the rotating coordinates fixed in the top. The Hamiltonian of the system is
Hence a state with quantum numbers J, m has energy
which gives the energy levels of the symmetric top.
(b) For the slightly asymmetric top the Hamiltonian is
Hence for the perturbed states:
(i) J = 0, m = 0, (nondegenerate):
(ii) J = 1, m = 0, (nondegenerate):
(iii) J = 1, m = fl, (two-fold degenerate):
As degeneracy occurs, we first calculate
which means that the energy of the states J = 1, m = h, E\(1,\pm 1\) splits into two levels: