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Related papers: New Collider Bound on Light Gravitino Mass

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The LEP experiments give a lower bound on the neutralino mass of about 46 GeV which, however, relies on a supersymmetric grand unification relation. Dropping this assumption, the experimental lower bound on the neutralino mass vanishes…

High Energy Physics - Phenomenology · Physics 2011-05-10 John A. Conley , Herbert K. Dreiner , Peter Wienemann

When SUSY breaking produces only dimension-2 operators, gluino and photino masses are of order 1 GeV or less. The gluon-gluino bound state has mass 1.3-2.2 GeV and lifetime > 10^{-5} - 10^{-10} s. This range of mass and lifetime is largely…

High Energy Physics - Phenomenology · Physics 2008-11-26 Glennys R. Farrar

Recent results obtained by the D0 Collaboration on searches for squarks and gluinos in proton-antiproton collisions at sqrt(s) =1.96 TeV at the Fermilab Tevatron collider are discussed. For the inclusive searches, events with multiple jets…

High Energy Physics - Experiment · Physics 2008-10-15 Krisztian Peters

A search for supersymmetry is presented in events with a single charged lepton, electron or muon, and multiple hadronic jets. The data correspond to an integrated luminosity of 138 fb$^{-1}$ of proton-proton collisions at a center-of-mass…

High Energy Physics - Experiment · Physics 2023-09-28 CMS Collaboration

A generic feature of gauge-mediated supersymmetry breaking models is that the gravitino is the lightest supersymmetric particle (LSP). In order not to overclose the universe, the gravitino LSP should be light enough (~ 1 keV), or…

High Energy Physics - Phenomenology · Physics 2009-11-10 Gi-Chol Cho , Yosuke Uehara

We reanalyze the constraints on light gluinos (m_{\tilde{g}}\leq 5 GeV/c^2) from the hadronic Z decays into four jets. We find that the published OPAL data from the 1991 and 1992 runs exclude a light quasi-stable gluino with mass \lesssim…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andre de Gouvea , Hitoshi Murayama

We study bound-state effects on the pair production of gluinos at hadron colliders, in a context of the minimal supersymmetric extension of the standard model. Due to the expected large mass and the octet color-charge of gluinos, the…

High Energy Physics - Phenomenology · Physics 2009-12-07 Kaoru Hagiwara , Hiroshi Yokoya

A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\sqrt{s}$ = 8 TeV data set collected…

High Energy Physics - Experiment · Physics 2015-10-22 ATLAS Collaboration

A search for squarks and gluinos in final states containing hadronic jets, missing transverse momentum but no electrons or muons is presented. The data were recorded in 2015 by the ATLAS experiment in $\sqrt{s}=$ 13 TeV proton--proton…

High Energy Physics - Experiment · Physics 2016-12-14 ATLAS Collaboration

Grand-unified models with extra dimensions at the GUT scale will typically contain exotic states with Standard Model charges and GUT-scale masses. They can act as messengers for gauge-mediated supersymmetry breaking. If the number of…

High Energy Physics - Phenomenology · Physics 2015-05-28 F. Brümmer , W. Buchmüller

A search for the weak production of charginos and neutralinos into final states with three electrons or muons and missing transverse momentum is presented. The analysis uses 2.06 fb^-1 of sqrt(s) = 7 TeV proton-proton collision data…

High Energy Physics - Experiment · Physics 2012-08-27 ATLAS Collaboration

The light gaugino scenario predicts that the lighter chargino mass is less than m_W, gluino and lightest neutralino masses are <~ 1 GeV, and the dominant decay mode of charginos and non-LSP neutralinos is generically to three jets. The…

High Energy Physics - Phenomenology · Physics 2007-05-23 Glennys R. Farrar

We report the result of a search for charginos and neutralinos, in e+e- collisions at 189 GeV centre-of-mass energy at LEP. No evidence for such particles is found in a data sample of 176 pb^{-1}. Improved upper limits for these particles…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

A search for supersymmetry involving the pair production of gluinos decaying via third-generation squarks into the lightest neutralino ($\displaystyle\tilde\chi^0_1$) is reported. It uses LHC proton-proton collision data at a centre-of-mass…

High Energy Physics - Experiment · Physics 2018-07-27 ATLAS Collaboration

We consider the neutralino mass matrix in a supersymmetric theory based on SU(2) $\times$ U(1) gauge group with arbitrary number of singlet, doublet and triplet Higgs superfields. We derive an upper bound on the mass of the lightest…

High Energy Physics - Phenomenology · Physics 2008-02-03 P. N. Pandita

In this letter we have presented a novel version of "long-lived" gluinos in supersymmetric models with the gluino the lightest ordinary supersymmetric particle [LOSP] and axino LSP. Within certain ranges of the axion decay constant $f_a < 1…

High Energy Physics - Phenomenology · Physics 2015-12-09 Stuart Raby

In models of low-energy gauge mediation, the observed Higgs mass is in tension with the cosmological limit on the gravitino mass $m_{3/2} \lesssim 16$ eV. We present an alternative mediation mechanism of supersymmetry breaking via a $U(1)$…

High Energy Physics - Phenomenology · Physics 2015-07-15 Anson Hook , Hitoshi Murayama

In the LHC searches for gluinos it is usually assumed that they decay predominantly into the lightest neutralino plus jets. In this work we perform a proof-of-concept collider analysis of a novel supersymmetric signal in which gluinos decay…

High Energy Physics - Phenomenology · Physics 2021-09-15 Ernesto Arganda , Antonio Delgado , Roberto A. Morales , Mariano Quirós

Present data indicates that the gluino (if it exists) must be heavier than about 95~GeV. During the next few years as the Tevatron integrated luminosity increases, gluino searches will be able to probe the mass range between 100 and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Howard E. Haber

Uncertainties of the MSSM predictions are due to an unknown SUSY breaking mechanism. To reduce these uncertainties, one usually imposes constraints on the MSSM parameter space. Recently, two new constraints became available, both from…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Yu. Bogachev , A. V. Gladyshev , D. I. Kazakov , A. S. Nechaev
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