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Related papers: Light Gluino and Tevatron Data

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The effects of light, long-lived gluinos on $2\to 2$ processes at hadron colliders are examined. Such particles can mediate single squark resonant production via $q\glu\to\sq\to q\glu$ which would significantly modify the dijet data sample.…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Hewett , T. Rizzo , M. Doncheski

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

We consider the possibility that the lightest supersymmetric particle is a heavy gluino. After discussing models in which this is the case, we demonstrate that the gluino-LSP could evade cosmological and other constraints by virtue of…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Baer , K. Cheung , J. F. Gunion

We calculate the production cross-sections for the vector and pseudoscalar bound states of two gluinos. It is shown that existing and future colliders imply a realistic chance of observing gluinonium as a narrow peak in the two-jet…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Chikovani , V. Kartvelishvili , R. Shanidze , G. Shaw , .

In supergravity theories with a very light gravitino, the gluino decays dominantly to a gluon and a gravitino. This results in a much larger missing $E_T$ for the multijet final states in hadronic colliders. We use the latest Tevatron data…

High Energy Physics - Phenomenology · Physics 2009-10-30 Duane A. Dicus , S. Nandi

The results of a search for gluinos in final states with an isolated electron or muon, multiple jets and large missing transverse momentum using proton--proton collision data at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV are presented.…

High Energy Physics - Experiment · Physics 2016-11-11 ATLAS Collaboration

The scenario of light gluinos and light sbottoms was advocated to explain the discrepancy between the measured and theoretical production of $b$ quarks at the Tevatron. This scenario will have model-independent predictions for $Z\to q\bar q…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kingman Cheung , Wai-Yee Keung

We argue that a relatively light massive gluon with mass <= 1 TeV, small purely axial couplings to light quarks and sizable vector and axial couplings to the top quark can reproduce the large forward-backward asymmetry observed at the…

High Energy Physics - Phenomenology · Physics 2011-08-09 Roberto Barcelo , Adrian Carmona , Manuel Masip , Jose Santiago

Parton distribution functions for protons are devised in which a light gluino is included along with standard model quark, antiquark, and gluon constituents. A global analysis of a large set of hadronic scattering data provides empirical…

High Energy Physics - Phenomenology · Physics 2007-05-23 Edmond L. Berger

It is shown that if the sneutrino is the second lightest SUSY particle, then the decay products of squarks and gluinos produced at the TEVATRON collider tend to have i) more leptons, ii) smaller number of jets and iii) two or more carriers…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amitava Datta , Monoranjan Guchait , Nirmalaya Parua

A search for squarks and gluinos in final states containing high-$p_{\rm T}$ jets, missing transverse momentum and no electrons or muons is presented. The data were recorded in 2012 by the ATLAS experiment in $\sqrt{s}=8$ TeV proton-proton…

High Energy Physics - Experiment · Physics 2014-10-07 ATLAS Collaboration

We searched for the appearance of pi+pi- pairs with invariant mass greater than 648 MeV in a neutral beam. Such an observation could signify the decay of a long-lived light neutral particle. We find no evidence for this decay. Our null…

High Energy Physics - Experiment · Physics 2008-11-26 J. Adams

We investigate the collider phenomenology of gluino-bino co-annihilation scenario both at the Tevatron and 7 TeV LHC. This scenario can be realized, for example, in a class of realistic supersymmetric models with non-universal gaugino…

High Energy Physics - Phenomenology · Physics 2011-01-27 M. Adeel Ajaib , Tong Li , Qaisar Shafi , Kai Wang

If the gravitino (G) is very light and all the other supersymmetric particles are above threshold, supersymmetry may still be found at colliders, by looking at processes with only gravitinos and ordinary particles in the final state. We…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. Brignole , F. Feruglio , M. L. Mangano , F. Zwirner

We search for physics beyond the standard model using events with a photon, two or more hadronic jets, and an apparent imbalance in transverse energy, in $p\bar{p}$ collisions at the Fermilab Tevatron at $\sqrt{s}=1.8$ TeV. Such events are…

High Energy Physics - Experiment · Physics 2008-11-26 B. Abbott

The presence of a light b-squark (with mass about 4 GeV) and gluino (with mass about 15 GeV) might explain the observed excess in b-quark production at the Tevatron. Though provocative, this model is not excluded by present data. The light…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Becher , Stephan Braig , Matthias Neubert , Alexander L. Kagan

In supersymmetric models where the magnitude of the GUT scale gaugino mass parameter M_3 is suppressed relative to M_1 and M_2, the lightest neutralino can be a mixed higgsino-bino state with a thermal relic abundance in agreement with the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Howard Baer , Azar Mustafayev , Stefano Profumo , Xerxes Tata

In scenarios with relatively light down squarks, motivated, e.g., by SO(10) D terms, jets + missing $E_T$ signals can be observed at the luminosity upgraded Tevatron even if the squarks are much heavier than the gluinos and the common…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amitava Datta , Shyamapada Maity , Anindya Datta

In the framework of minimal supersymmetric model we examine the Z-peak constraints on the scenario of one light sbottom (2--5.5 GeV) and light gluino (12--16 GeV), which has been successfully used to explain the excess of bottom quark…

High Energy Physics - Phenomenology · Physics 2011-01-27 Junjie Cao , Zhaohua Xiong , Jin Min Yang

A low-energy supersymmetry scenario with a light gluino of mass 12 - 16 GeV and light sbottom (b1) of mass 2 - 6 GeV has been used to explain the apparent overproduction of b quarks at the Tevatron. In this scenario the other mass…

High Energy Physics - Phenomenology · Physics 2011-01-27 Rahul Malhotra
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