A representation theory for Lie groups is developed taking the Hilbert spac
e, say H-w, of the w*-algebra standard representation as the representation
space. In this context the states describing physical systems are amplitud
e wave functions but closely connected with the notion of the density matri
x. Then, based on symmetry properties, a general physical interpretation fo
r the dual variables of thermal theories, in particular the thermofield dyn
amics (TFD) formalism, is introduced. The kinematic symmetries, Galilei and
Poincare, are studied and (density) amplitude matrix equations are derived
for both of these cases. In the same context of group theory, the notion o
f phase space in quantum theory is analysed. Thus, in the non-relativistic
situation, the concept of density amplitude is introduced, and as an exampl
e, a spin-half system is algebraically studied; Wigner function representat
ions for the amplitude density matrices are derived and the connection of T
FD and the usual Wigner-function methods are analysed. For the Poincare sym
metries the relativistic density matrix equations are studied for the scala
r and spinorial fields. The relativistic phase space is built following the
lines of the non-relativistic case. So, for the scalar field, the kinetic
theory is introduced via the Klein-Gordon density-matrix equation, and a de
rivation of the Juttiner distribution is presented as an example, thus maki
ng it possible to compare with the standard approaches. The analysis of the
phase space for the Dirac field is carried out in connection with the dual
spinor structure induced by the Dirac-field density-matrix equation, with
the physical content relying on the symmetry groups. Gauge invariance is co
nsidered and, as a basic result, it is shown that the Heinz density operato
r (which has been used to develope a gauge covariant kinetic theory) is a p
articular solution for the (Klein-Gordon and Dirac) density-matrix equation
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