In thermal field dynamics, thermal states are obtained from restrictio
ns of vacuum states on a doubled field algebra. It is shown that the s
uitably doubled Fock representations of the Heisenberg algebra do not
need to be introduced by hand but can be canonically handed down from
deformations of the extended Heisenberg bialgebra. No artificial redef
initions of fields are necessary to obtain the thermal representations
and the case of arbitrary dimension is considered from the beginning.
Our results support a possibly fundamental role of bialgebra structur
es in defining a general framework for thermal field dynamics. (C) 199
7 American Institute of Physics.