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Duality-invariant Quantum Field Theories of Charges and Monopoles

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arxiv hep-th/9906079 v1 pith:DIHMBW6W submitted 1999-06-10 hep-th

classification hep-th
keywords fieldquantumtheorychargesclassicalactionconditiondirac-schwinger
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We present a manifestly Lorentz- and SO(2)-Duality-invariant local Quantum Field Theory of electric charges, Dirac magnetic monopoles and dyons. The manifest invariances are achieved by means of the PST-mechanism. The dynamics for classical point particles is described by an action functional living on a circle, if the Dirac-Schwinger quantization condition for electric and magnetic charges holds. The inconsistent classical field theory depends on an arbitrary, but fixed, external vector field, a generalization of the Dirac-string. Nevertheless, the Quantum Field Theory, obtained from this classical action via a functional integral approach, turns out to be independent of the particular vector field chosen, and thus consistent, if the Dirac-Schwinger quantization condition holds. We provide explicit expressions for the generating functionals of observables, proving that they are Dirac-string independent. Since Lorentz-invariance is manifest at each step, the quantum theory admits also a manifestly diffeomorphism invariant coupling to external gravity. Relations with previous formulations, and with SO(2)--non invariant theories are clarified.

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  1. Coupling Self-Dual p-Form Gauge Fields to Self-Dual Branes

    hep-th 2025-01 conditional novelty 5.0 of 10

    Self-dual p-form gauge fields in d=4k+2 dimensions can be coupled to self-dual branes via Dirac branes, with the action invariant under Dirac brane deformations subject to the Dirac veto.

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