Local Charged States of the Gauge Field in Three Dimensional Maxwell-Type Theories

Details Local Charged States of the Gauge Field in Three Dimensional Maxwell-Type Theories Local Charged States of the Gauge Field in Three Dimensional Maxwell-Type Theories

1996-03-27

arxiv.org/abs/hep-th/9603180v1

Mod.Phys.Lett. A11 (1996) 1985-1998

Physics

High Energy Physics

High Energy Physics - Theory

Latex, 16 pages, two figures available upon request as postscript files

Scientific paper

Gauge invariant local creation operators of charged states are introduced and studied in pure gauge theories of the Maxwell type in 2+1D. These states are usually unphysical because of the subsidiary condition imposed on the physical subspace by Gauss' law. A dual Maxwell theory which possesses a topological electric charge is introduced. Pure Electrodynamics lies in the sector where the topological charge identically vanishes. Charge bearing operators fully expressed in terms of the gauge field, however, can create physical states in the nontrivial topological sectors which thereby generalize QED. An order disorder structure exists relating the charged operators and the magnetic flux creating (vortex) operators, both through commutation rules and correlation functions. The relevance of this structure for bosonization in 2+1D is discussed.

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