  We investigate in this article the long-time behaviour of the solutions to
the energy-dependant, spatially-homogeneous, inelastic Boltzmann equation for
hard spheres. This model describes a diluted gas composed of hard spheres under
statistical description, that dissipates energy during collisions. We assume
that the gas is "anomalous", in the sense that energy dissipation increases
when temperature decreases. This allows the gas to cool down in finite time. We
study existence and uniqueness of blow up profiles for this model, together
with the trend to equilibrium and the cooling law associated, generalizing the
classical Haff's Law for granular gases. To this end, we investigate the
asymptotic behaviour of the inelastic Boltzmann equation with and without drift
term by introducing new strongly "nonlinear" self-similar variables.
