In a diatomic gas, there are three degrees of freedom of rotation, of which the frozen mode (the rotation around the bond axis) is ruled out because the energy spacing of frozen rotational energies is about 100 000 times as great as the other two, non-frozen rotations (around the axes perpendicular to the bond axes).
But what if the temperature of the gas is very high (just beneath the temperature at which the molecular bonds start breaking up)? The two "normal" rotations possess an energy which grows quadratically with n, the number of angular momentum quanta ($L=\frac{nh}{2\pi}$): $T=\frac{n^2h^2}{8\pi^2I}$ (T is the kinetic energy, I the moment of inertia and h is Planck's constant). So if the molecule possesses 100 quanta (n=100) of angular momentum (for the "normal" rotations), the energy gets bigger 100 000 times as in the case n=1 (of course, the same is true for the frozen rotation).
Are the non-frozen rotational energies high enough before the molecular breakup to convey quanta of angular momentum to the two atoms in a "target" molecule, and give this molecule an angular momentum around the bond axis (n=1), in which case the equipartition theorem holds?