  We propose a non-abelian higher-spin theory in two dimensions for an infinite
multiplet of massive scalar fields and infinitely many topological higher-spin
gauge fields together with their dilaton-like partners. The spectrum includes
local degrees of freedom although the field equations take the form of flatness
and covariant constancy conditions because fields take values in a suitable
extension of the infinite-dimensional higher-spin algebra $hs[\lambda]$. The
corresponding action functional is of BF-type and generalizes the known
topological higher-spin Jackiw-Teitelboim gravity.
