The large time behavior of non-negative solutions to the viscous
Hamilton-Jacobi equation ut−Δu+∣∇u∣q=0 in the whole space
RN is investigated for the critical exponent q=(N+2)/(N+1). Convergence
towards a rescaled self-similar solution of the linear heat equation is shown,
the rescaling factor being (log(t))−(N+1). The proof relies on the
construction of a one-dimensional invariant manifold for a suitable truncation
of the equation written in self-similar variables.Comment: 17 pages, no figur