Supersymmetric Models with Higher Dimensional Operators

dc.creatorAntoniadis, I.
dc.creatorDudas, E.
dc.creatorGhilencea, D. M.
dc.date2007-08-02
dc.date2008-03-03
dc.date.accessioned2026-07-07T12:59:15Z
dc.date.available2026-07-07T12:59:15Z
dc.descriptionIn 4D renormalisable theories, integrating out massive states generates in the low energy effective action higher dimensional operators (derivative or otherwise). Using a superfield language it is shown that a 4D N=1 supersymmetric theory with higher derivative operators in either the Kahler or the superpotential part of the Lagrangian and with an otherwise arbitrary superpotential, is equivalent to a 4D N=1 theory of second order (i.e. without higher derivatives) with additional superfields and renormalised interactions. We provide examples where a free theory with trivial supersymmetry breaking provided by a linear superpotential becomes, in the presence of higher derivatives terms and in the second order version, a non-trivial interactive one with spontaneous supersymmetry breaking. The couplings of the equivalent theory acquire a threshold correction through their dependence on the scale of the higher dimensional operator(s). The scalar potential in the second order theory is not necessarily positive definite, and one can in principle have a vanishing potential with broken supersymmetry. We provide an application to MSSM and argue that at tree-level and for a mass scale associated to a higher derivative term in the TeV range, the Higgs mass can be lifted above the current experimental limits.
dc.description36 pages; some clarifications and references added
dc.identifierhttps://arxiv.org/abs/0708.0383
dc.identifierhttp://arxiv.org/abs/0708.0383
dc.identifierJHEP 0803:045,2008
dc.identifierdoi:10.1088/1126-6708/2008/03/045
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/225514
dc.subjectHigh Energy Physics - Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleSupersymmetric Models with Higher Dimensional Operators
dc.typetext

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