6.
Noether's first theorem tells us that the global symmetry group
G
r
of an action integral is a Lie group of point transformations that acts on the Cartesian product of the space-time manifold with the space of states and their derivatives. Gauge theory constructs are thus required for symmetry groups that act indiscriminately on the independent and dependent variables where the group structure can not necessarily be realized as a subgroup of the general linear group. Noting that the Lie algebra of a general symmetry group
G
r
can be realized as a Lie algebra
g
r
of Lie derivatives on an appropriately structured manifold,
G
r
-covariant derivatives are introduced through study of connection 1-forms that take their values in the Lie algebra
g
r
of Lie derivatives (operator-valued connections). This leads to a general theory of operator-valued curvature 2-forms and to the important special class of Lie connections. The latter are naturally associated with the minimal replacement and minimal coupling constructs of gauge theory when the symmetry group
G
r
is allowed to act locally. Lie connections give rise to the gauge fields that compensate for the local action of
G
r
in a natural way. All governing field equations and their integrability conditions are derived for an arbitrary finite dimensional Lie group of symmetries. The case where
G
r
contains the ten-parameter Poincaré group on a flat space-time
M
4 is considered. The Lorentz structure of
M
4 is shown to give a pseudo-Riemannian structure of signature 2 under the minimal replacement associated with the Lie connection of the local action of the Poincaré group. Field equations for the matter fields and the gauge fields are given for any system of matter fields whose action integral is invariant under the global action of the Poincaré group.
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