Chern-Simons D=3, N=6 superfield theory

dc.creatorZupnik, B. M.
dc.date2007-11-29
dc.date2007-12-13
dc.date.accessioned2026-07-07T11:13:27Z
dc.date.available2026-07-07T11:13:27Z
dc.descriptionWe construct the D=3, N=5 harmonic superspace using the SO(5)/U(1) x U(1) harmonics. Three gauge harmonic superfields satisfy the off-shell constraints of the Grassmann and harmonic analyticities. The corresponding component supermultiplet contains the gauge field A_m and an infinite number of bosonic and fermionic fields with the SO(5) vector indices arising from decompositions of gauge superfields in harmonics and Grassmann coordinates. The nonabelian superfield Chern-Simons action is invariant with respect to the N=6 superconformal supersymmetry realized on the N=5 superfields. The component Lagrangian contains the Chern-Simons interaction of A_m and an infinite number of bilinear and trilinear interactions of auxiliary fields. The fermionic and bosonic auxiliary fields from the infinite N=5 multiplet vanish on-shell.
dc.descriptionLatex file, 9 pages, v.2 a note and references added
dc.identifierhttps://arxiv.org/abs/0711.4680
dc.identifierhttp://arxiv.org/abs/0711.4680
dc.identifierPhys.Lett.B660:254-259,2008
dc.identifierdoi:10.1016/j.physletb.2007.12.052
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/191721
dc.subjectHigh Energy Physics - Theory
dc.titleChern-Simons D=3, N=6 superfield theory
dc.typetext

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