Equivalence of partition functions for noncommutative U(1) gauge theory and its dual in phase space

Simple item page
dc.creatorDayi, O. F.
dc.creatorYapiskan, B.
dc.date2004-07-30
dc.date2004-11-25
dc.date.accessioned2026-07-07T10:50:07Z
dc.date.available2026-07-07T10:50:07Z
dc.descriptionEquivalence of partition functions for U(1) gauge theory and its dual in appropriate phase spaces is established in terms of constrained hamiltonian formalism of their parent action. Relations between the electric--magnetic duality transformation and the (S) duality transformation which inverts the strong coupling domains to the weak coupling domains of noncommutative U(1) gauge theory are discussed in terms of the lagrangian and the hamiltonian densities. The approach presented for the commutative case is utilized to demonstrate that noncommutative U(1) gauge theory and its dual possess the same partition function in their phase spaces at the first order in the noncommutativity parameter θ.
dc.description15 pages. Version to appear in JHEP
dc.identifierhttps://arxiv.org/abs/hep-th/0407269
dc.identifierhttp://arxiv.org/abs/hep-th/0407269
dc.identifierJHEP0411:064,2004
dc.identifierdoi:10.1088/1126-6708/2004/11/064
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/184441
dc.subjectHigh Energy Physics - Theory
dc.titleEquivalence of partition functions for noncommutative U(1) gauge theory and its dual in phase space
dc.typetext

Files

Collections

arXiv