“…Of particular importance are the integrable cases of the rigid body problem [9,10], which include the free asymmetric top (Euler top) [1,4,6], the symmetric top in a uniform external gravitational field (Lagrange top) [6,11], and the Kovalevskaya top [6,12]. The theory of rigid body motion also provides the basis for analysis and interpretation of the rotational dynamics and spectra of semi-rigid molecules [2,5,13,14,15,16]. In molecular terms the Euler top is simply a free asymmetric top molecule [5,14,15], the Lagrange top models a symmetric top molecule with a dipole moment in an electric field [15,17], while there does not appear to be an obvious molecular analogue for the Kovalevskaya top.…”