The extension of the Kramers
theory of the
escape rate of a Brownian particle from a potential well to the entire range of damping proposed by Mel’nikov and Meshkov [V.I. Mel’nikov, S.V. Meshkov, J. Chem. Phys. 85 (1986) 1018] is applied to the inertial rotational Brownian motion of a fixed axis rotator in a potential
V(θ)=−K1cos2θ−K2cos4θ, where
θ is the angle specifying the orientation of the rotator and
K1 and
K2 are constants. It is shown that in the neighbourhood of
K1
4K2 (flat barrier), the Mel’nikov–Meshkov method must suitably be adapted so that the effect of a nonparabolic barrier top can be correctly accounted for in the calculation of the relaxation time. The results obtained are compared with numerical calculations of the longest relaxation time (inverse smallest nonvanishing eigenvalue) using a matrix continued fraction algorithm and reasonable agreement is obtained for
K1≥4K2 and all values of the dissipation parameter.