  Inelastic light scattering from Dirac-type electrons in graphene is shown to
be dominated by the generation of the inter-band electronic modes which are odd
in terms of time-inversion symmetry and belong to the irreducible
representation A$_2$ of the point group C$_{6v}$ of the honeycomb crystal. At
high magnetic fields, these electron-hole excitations appear as peculiar $n^-
\to n^+$ inter-Landau-level modes with energies $\omega_n=2\sqrt{2n} \hbar
v/\lambda_B$ and characteristically crossed polarisation of in/out photons.
