  Gauge fields of mixed symmetry, corresponding to arbitrary representations of
the local Lorentz group of the background spacetime, arise as massive modes in
compactifications of superstring theories. We describe bosonic gauge field
theories on constant curvature spaces whose fields are in irreducible
representations of the general linear group corresponding to Young tableaux
with two columns. The gauge-invariant actions for such fields are given and
generally require the use of auxiliary fields and additional mass-like terms.
We examine these theories in various (partially) massless regimes in which each
of the mass-like parameters vanishes. We also make some comments about how the
structure extends for gauge fields corresponding to arbitrary Young tableaux.
