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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 2009-10-30 Andrea Brignole , Ferruccio Feruglio , Fabio Zwirner

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

Searches for final states expected in models with light gravitinos have been performed, including experimental topologies with multi-leptons with missing energy, leptons and photons with missing energy, and jets and photons with missing…

High Energy Physics - Experiment · Physics 2008-11-26 The OPAL collaboration , G. Abbiendi

If supersymmetry is spontaneously at a low energy scale then the resulting gravitino would be very light. The interaction strength of the longitudinal components of such a light gravitino to electron-selectron pair then becomes comparable…

High Energy Physics - Phenomenology · Physics 2009-10-31 Uma Mahanta

In supergravity models with low supersymmetry breaking scale the gravitinos can be superlight with mass in the micro-eV to keV range. In such a case, gravitino emission provides a new cooling mechanism for protoneutron stars and therefore…

High Energy Physics - Phenomenology · Physics 2014-11-17 Duane A. Dicus , Rabindra N. Mohapatra , Vigdor L. Teplitz

We present cross sections for the production of the lightest supersymmetric particle as a neutralino state in the minimal supersymmetric standard model at electron-photon colliders. The lightest supersymmetric particle mass is taken at a…

High Energy Physics - Phenomenology · Physics 2009-10-22 Heinz König , K. A. Peterson

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

Results are reported from a search for supersymmetry with gauge-mediated supersymmetry breaking in electroweak production. Final states with photons and large missing transverse energy (MET) were examined. The data sample was collected in…

High Energy Physics - Experiment · Physics 2016-07-29 CMS Collaboration

Light gravitino productions in association with a neutralino (selectron) in e^+e^- (e^-\gamma) collisions are restudied in a scenario that the lightest supersymmetric particle is a gravitino and the produced neutralino (selectron) promptly…

High Energy Physics - Phenomenology · Physics 2015-05-28 K. Mawatari , B. Oexl , Y. Takaesu

We search for inclusive high $E_T$ diphoton events with large missing transverse energy in $p\bar{p}$ collisions at $\sqrt{s}$=1.8 TeV. Such events are expected from pair production of charginos and neutralinos within the framework of the…

High Energy Physics - Experiment · Physics 2016-08-31 Dzero Collaboration , B. Abbott

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

The exclusive gamma-met signal has a small standard model cross-section and is thus a good channel in which to look for signs of new physics. This signature is predicted by models with a superlight gravitino or with large extra spatial…

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

In some supergravity models, the superlight gravitino is accompanied by a light weakly coupled scalar (S) and pseudo-scalar (P) particle. The coupling of these particles to matter is inversely proportional to the product of the gravitino…

High Energy Physics - Phenomenology · Physics 2009-10-30 J. A. Grifols , R. N. Mohapatra , A. Riotto

We consider, in the context of the minimal supersymmetric standard model, the case where the gravitino weighs 10^6 GeV or more, which is preferred by various cosmological difficulties associated with unstable gravitinos. Despite the large…

High Energy Physics - Phenomenology · Physics 2015-06-03 Kwang Sik Jeong , Masatoshi Shimosuka , Masahiro Yamaguchi

The effect of spin-0 goldstino superpartners is considered on the nucleosynthesis bounds arising when a superlight gravitino appears as an effective massless neutrino species. When the scalar and pseudoscalar superpartners are relativistic…

High Energy Physics - Phenomenology · Physics 2009-10-30 Tony Gherghetta

If supersymmetry is broken at TeV scale, particles from sector responsible for supersymmetry breaking - goldstino and sgoldstinos - can reveal themselves already at the LHC experiments. We discuss bounds on supersymmetry breaking scale from…

High Energy Physics - Phenomenology · Physics 2017-09-18 S. V. Demidov , I. V. Sobolev

Very light gravitinos could be produced at a sizeable rate at colliders and have been searched for in the mono-photon or mono-jet plus missing momentum signature. Strategies for enhancing the signal over background and interpretations of…

High Energy Physics - Phenomenology · Physics 2015-06-23 Fabio Maltoni , Antony Martini , Kentarou Mawatari , Bettina Oexl

Light gravitinos, with mass in the eV to MeV range, are well-motivated in particle physics, but their status as dark-matter candidates is muddled by early-Universe uncertainties. We investigate how upcoming data from colliders may clarify…

High Energy Physics - Phenomenology · Physics 2011-10-12 Jonathan L. Feng , Marc Kamionkowski , Samuel K. Lee

The experimental signatures for low energy supersymmetry breaking are presented. The lightest standard model superpartner is unstable and decays to its partner plus a Goldstino, $G$. For a supersymmetry breaking scale below a few 1000 TeV…

High Energy Physics - Phenomenology · Physics 2009-10-28 Savas Dimopoulos , Michael Dine , Stuart Raby , Scott Thomas , James D. Wells

Recently, a scenario has been proposed in which the gravitational scale could be as low as the TeV scale, and extra dimensions could be large and detectable at the electroweak scale. Although supersymmetry is not a requirement of this…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Atwood , C. P. Burgess , E. Filotas , F. Leblond , D. London , I. Maksymyk
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