2000
DOI: 10.1088/0305-4470/33/5/315
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The physical projector and topological quantum field theories:U(1) Chern-Simons theory in 2 + 1 dimensions

Abstract: The recently proposed physical projector approach to the quantisation of gauge invariant systems is applied to the U(1) Chern-Simons theory in 2+1 dimensions as one of the simplest examples of a topological quantum field theory. The physical projector is explicitely demonstrated to be capable of effecting the required projection from the initially infinite number of degrees of freedom to the finite set of gauge invariant physical states whose properties are determined by the topology of the underlying manifold. Show more

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Cited by 6 publications
(13 citation statements)
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“…The nonperturbative solution of the Schwinger model (a U(1) gauge invariant field theory coupled to a massless fermion in 1+1 dimensions) has also been recovered through the physical projector without the necessaity of any gauge fixing. [33] Likewise, the physical projector has been applied [34] to the quantization of the U(1) invariant Chern-Simons theory, one of the simplest topological quantum field theories in which only a finite number of gauge invariant states, dependent only on the differential topology of the spacetime manifold but not its geometry, is to be projected out from an infinite set of quantum states. These successes thus bode well for the relevance of this recent approach towards the quantization of constrained dynamics.…”
Section: Klauder's Physical Projector: Gauge Invariant Quantum Dynamimentioning
confidence: 99%
“…The nonperturbative solution of the Schwinger model (a U(1) gauge invariant field theory coupled to a massless fermion in 1+1 dimensions) has also been recovered through the physical projector without the necessaity of any gauge fixing. [33] Likewise, the physical projector has been applied [34] to the quantization of the U(1) invariant Chern-Simons theory, one of the simplest topological quantum field theories in which only a finite number of gauge invariant states, dependent only on the differential topology of the spacetime manifold but not its geometry, is to be projected out from an infinite set of quantum states. These successes thus bode well for the relevance of this recent approach towards the quantization of constrained dynamics.…”
Section: Klauder's Physical Projector: Gauge Invariant Quantum Dynamimentioning
confidence: 99%
“…When restricted to the physical subspace for which these constraints are satisfied, the above gauge invariant Hamiltonian reduces to a functional depending only on the dynamical physical sector, given by the expression in the first line of (20).…”
Section: The Physical-topological (Pt) Factorisationmentioning
confidence: 99%
“…Our redefinition of fields deals with the original degrees of freedom in such a way that within the Hamiltonian formalism, non propagating (and gauge variant) degrees of freedom are decoupled from the dynamical sector. This latter sector describes only physical degrees of freedom, namely the gauge invariant canonically conjugate electric fields, which diagonalise the physical Hamiltonian (20) in such a way that they acquire a mass through a mixing of the original variables (18). However the Poisson bracket structure remains unaffected since these field redefinitions define merely a canonical transformation.…”
Section: The Physical-topological (Pt) Factorisationmentioning
confidence: 99%
“…In addition, Klauder [19] has applied the projection operator method in a study of quantum gravity. Finally, a U(1) Chern-Simons model has been studied and solved with the projection operator method using coherent states in [34].…”
Section: Other Applications Of the Pro-jection Operator Approachmentioning
confidence: 99%