Impact of LHC Searches on NLSP Top Squark and Gluino Mass
arXiv:1112.4461 · doi:10.1007/JHEP05(2012)148
Abstract
We explore the implications of 7 TeV LHC searches for a scenario in which one of the stops is the next-to lightest supersymmetric particle (NLSP). The NLSP stop (\tilde{t}_1) is assumed to decay exclusively into neutralino and charm quark. We consider processes where the stops are pair produced together with a hard QCD jet. We also consider stop quarks from gluino decays, \tilde{g}\to t\tilde{t}_1^\ast+\bar{t}\tilde{t}_1. We show that the monojet ATLAS and CMS searches corresponding to 1 fb^{-1} of integrated luminosity are sensitive to stop masses of up to 160 GeV, with the 20% neutralino-stop coannihilation region essentially ruled out for M_{\tilde{t}_1}\lesssim 140 GeV. The region M_{\tilde{t}_1}\lesssim 130 GeV is excluded with even relatively larger mass difference, M_{\tilde{t}_1}-M_{\tildeχ_1^0}\sim 40 GeV, by the multi-jets search. The b-jet and same-sign dilepton searches are sensitive to a heavier gluino because they only pick up gluino pair production events followed by top quarks decaying into b-jets and same-sign dileptons, respectively. We find that the LHC data places a lower limit on the gluino mass in this scenario of about 600 GeV (700 GeV) from b-jets (same-sign dileptons) searches.
18 pages, 10 figures and 4 tables
References in corpus (14)
- PYTHIA 6.4 Physics and Manual
- Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions
- Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in sqrt(s) = 7 TeV proton-proton collisions
- Search for Supersymmetry at the LHC in Events with Jets and Missing Transverse Energy
- SUSY, the Third Generation and the LHC
- QCD radiation in the production of heavy colored particles at the LHC
- Searching for Directly Decaying Gluinos at the Tevatron
- The Status of GMSB After 1/fb at the LHC
- Heavy Flavor Simplified Models at the LHC
- Light Stop Searches at the LHC in Events with One Hard Photon or Jet and Missing Energy
- Light Stop NLSPs at the Tevatron and LHC
- Light Stop Decay in the MSSM with Minimal Flavour Violation
- Constraints on supersymmetry with light third family from LHC data
- Same-sign top quarks as signature of light stops
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- A Heavy SM-like Higgs and a Light Stop from Yukawa-Deflected Gauge Mediation
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- Exploring QCD uncertainties when setting limits on compressed SUSY spectra
- Very Light Scalar Top Quarks at the LHC
- NLSP Gluino and NLSP Stop Scenarios from b-tau Yukawa Unification
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- Improving the sensitivity of stop searches with on-shell constrained invariant mass variables
- A Toolkit of the Stop Search via the Chargino Decay
- Complementarity of WIMP Sensitivity with direct SUSY, Monojet and Dark Matter Searches in the MSSM
- Spot the stop with a b-tag
- Higgs Boson Production and Decay: Effects from Light Third Generation and Vectorlike Matter
- Boosted di-boson from a mixed heavy stop
- Stop and sbottom search using dileptonic variable and boosted top technique at the LHC
- Probing the flavor violating scalar top quark signal at the LHC
- Stop on Top: SUSY Parameter Regions, Fine-Tuning Constraints
- Automated third generation squark production to next-to-leading order
- Gluino Coannihilation and Observability of Gluinos at LHC RUN II
- Top jets as a probe of degenerate stop-NLSP LSP scenario in the framework of cMSSM
- Sparticle Spectroscopy from SO(10) GUT with a Unified Higgs Sector
- Demystifying the compressed top squark region with kinematic variables
- Effects of Neutrino Inverse Seesaw Mechanism on the Sparticle Spectrum in CMSSM and NUHM2
- Closing in on compressed gluino-neutralino spectra at the LHC