Prospects for Yukawa Unified SO(10) SUSY GUTs at the CERN LHC

dc.creatorBaer, Howard
dc.creatorKraml, Sabine
dc.creatorSekmen, Sezen
dc.creatorSummy, Heaya
dc.date2008-09-03
dc.date.accessioned2026-07-07T13:12:26Z
dc.date.available2026-07-07T13:12:26Z
dc.descriptionThe requirement of t-b-τYukawa coupling unification is common in simple grand unified models based on the gauge group SO(10), and it also places a severe constraint on the expected spectrum of superpartners. For Yukawa-unified models with μ>0, the spectrum is characterized by three mass scales: {\it i}). first and second generation scalars in the multi-TeV range, {\it ii}). third generation scalars, μand m_A in the few-TeV range and {\it iii}). gluinos in the \sim 350-500 GeV range with chargino masses around 100-160 GeV. In such a scenario, gluino pair production should occur at large rates at the CERN LHC, followed by gluino three-body decays into neutralinos or charginos. Discovery of Yukawa-unified SUSY at the LHC should hence be possible with only 1 fb^{-1} of integrated luminosity, by tagging multi-jet events with 2--3 isolated leptons, without relying on missing E_T. A characteristic dilepton mass edge should easily be apparent above Standard Model background. Combining dileptons with b-jets, along with the gluino pair production cross section information, should allow for gluino and neutralino mass reconstruction. A secondary corroborative signal should be visible at higher integrated luminosity in the W1Z2-> 3\ell channel, and should exhibit the same dilepton mass edge as in the gluino cascade decay signal.
dc.description25 pages including 18 EPS figures
dc.identifierhttps://arxiv.org/abs/0809.0710
dc.identifierhttp://arxiv.org/abs/0809.0710
dc.identifierJHEP 0810:079,2008
dc.identifierdoi:10.1088/1126-6708/2008/10/079
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/229578
dc.subjectHigh Energy Physics - Phenomenology
dc.titleProspects for Yukawa Unified SO(10) SUSY GUTs at the CERN LHC
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