The divergence of the heat conductivity in the thermodynamic limit is inves
tigated in 2d-lattice models of anharmonic solids with nearest-neighbour in
teraction from single-well potentials. Two different numerical approaches b
ased on nonequilibrium and equilibrium simulations protide consistent indic
ations in favour of a logarithmic divergence in "ergodic", i.e., highly cha
otic, dynamical regimes. Analytical estimates obtained in thr framework of
linear-responce theory confirm this finding, while tracing back the physica
l origin of this anomalous transport to the slow diffusion of the energy of
hydrodynamic modes, finally, numerical evidence of superanomalous transpor
t is given in the weakly chaotic regime, typically observed below a thresho
ld value of the energy density.