In the usual real-time finite-temperature gauge theory both the physic
al and the unphysical degrees of freedom are thermalised. We discuss t
he alternative approach where only the physical transverse components
of the gauge field have bare thermal propagators, whereas the unphysic
al degrees of freedom are not heated. We show how pinch singularities
are avoided: sometimes this requires resummation. If only the hard the
rmal loop is included in the resummation, the spatially-longitudinal c
omponent of the gauge field, which contains an extra collective plasmo
n mode, becomes fully thermalised, though the Faddeev-Popov ghost and
the remaining unphysical component of the gauge field remain frozen.