Testing Yukawa-unified SUSY during year 1 of LHC: the role of multiple b-jets, dileptons and missing E T

We examine the prospects for testing SO(10) Yukawa-unified supersymmetric models during the first year of LHC running at $ \sqrt s = 7\,{\text{TeV}} $ , assuming integrated luminosity values of ∼0.1-1 fb−1. We consider two cases: the Higgs splitting (HS) and the D-term splitting (DR3) models. Each generically predicts light gluinos and heavy squarks, with an inverted scalar mass hierarchy. We hence expect large rates for gluino pair production followed by decays to final states with large b-jet multiplicity. For 0.2 fb−1 of integrated luminosity, we find a 5σ discovery reach of $ {m_{\tilde g}} \sim 400\,{\text{GeV}} $ even if missing transverse energy, E T miss , is not a viable cut variable, by examining the multi-b-jet final state. A corroborating signal should stand out in the opposite-sign (OS) dimuon channel in the case of the HS model; the DR3 model will require higher integrated luminosity to yield a signal in the OS dimuon channel. This region may also be probed by the Tevatron with 5–10 fb−1 of data, if a corresponding search in the multi-b + E T miss channel is performed. With higher integrated luminosities of ∼1 fb−1, using E T miss plus a large multiplicity of b-jets, LHC should be able to discover Yukawa-unified SUSY with $ {m_{\tilde g}} \lesssim 630\,{\text{GeV}} $ . Thus, the year 1 LHC reach for Yukawa-unified SUSY should be enough to either claim a discovery of the gluino, or to very nearly rule out this class of models, since higher values of $ {m_{\tilde g}} $ lead to rather poor Yukawa unification.