Abstract
In computer studies of the Jahn–Teller system Γ8⊗τ2g, Thorson and Moffitt showed that periodic coalescences of the energy levels occur as the interaction between the electronic part Γ8 and the vibrational mode τ2g is increased. These near degeneracies have been analyzed by drawing a correspondence between the Γ8⊗τ2g system and a displaced one‐dimensional oscillator. It is shown that the degeneracies correspond to the zeros of the Bessel functions J1(z). In terms of the interaction parameter D and the oscillator number nτ of Thorson and Moffitt, z is 4D1/2(nτ+3/2)1/2 in the limit of large nτ. Second‐order effects have been cast in an analytic form and do not affect the existence of the degeneracies in that limit. Third‐order effects have also been studied. The theory is applied to the Jahn–Teller system E⊗ε.

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