  For a distribution advected by a simple chaotic map with diffusion, the
"strange eigenmode" is investigated from the Lagrangian (material) viewpoint
and compared to its Eulerian (spatial) counterpart. The eigenmode embodies the
balance between diffusion and exponential stretching by a chaotic flow. It is
not strictly an eigenmode in Lagrangian coordinates, because its spectrum is
rescaled exponentially rapidly.
