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We discuss the physics of a restricted Weyl symmetry in a curved space-time where a gauge parameter (x) of Weyl transformation satisfies a constraint =0. First, we present a model of QED where we have a restricted gauge symmetry in the sense that a U (1) gauge parameter (x) obeys a similar constraint =0 in a flat Minkowski space-time. Next, it is precisely shown that a global scale symmetry must be spontaneously broken at the quantum level. Finally, we discuss the origin of the restricted Weyl symmetry and show that its symmetry can be derived from a full Weyl symmetry by taking a gauge condition R=0 in the BRST formalism.
Ichiro Oda (Thu,) studied this question.