  Free massless fields of any spin in flat D-dimensional spacetime propagate at
the speed of light. But the retarded fields produced by the corresponding
point-like moving sources share this property only for even D. Since the
Green's functions of the d'Alembert equation are localized on the light cone in
even-dimensional spacetime, but not in odd dimensions, extraction of the
emitted part of the retarded field in odd D requires some care. We consider the
wave equations for spins 0, 1, and 2 in five-dimensional spacetime and analyze
the fall-off conditions for the retarded fields at large distances. It is shown
that the farthest part of the field contains a component propagating at the
speed of light, while the non-derivative terms propagate with all velocities up
to that of light. The generated radiation will contain a radiation tail
corresponding to the complete prehistory of the source's motion preceding the
retarded moment of time. We also demonstrate that dividing the Green's function
into a part localized on the light cone and another part that is not zero
inside the light cone gives separately the divergent terms in the Coulomb field
of a point source. Their sum, however, is finite and corresponds to the usual
power-law behaviour.
