6533b853fe1ef96bd12ac3e3

RESEARCH PRODUCT

METing SUSY on the Z peak

Vasiliki A MitsouO. VivesGabriela BarenboimE. RomeroJose Bernabeu

subject

PhysicsParticle physicsGluinoLarge Hadron ColliderPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetry01 natural sciencesStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutralinoGravitinoProduction (computer science)High Energy Physics::Experiment010306 general physicsEngineering (miscellaneous)Lepton

description

Recently the ATLAS experiment announced a 3 $\sigma$ excess at the Z-peak consisting of 29 pairs of leptons together with two or more jets, $E_T^{\rm miss}> 225$ GeV and $H_T \geq 600$ GeV, to be compared with $10.6 \pm 3.2$ expected lepton pairs in the Standard Model. No excess outside the Z-peak was observed. By trying to explain this signal with SUSY we find that only relatively light gluinos, $m_{\tilde g} \lesssim 1.2$ TeV, together with a heavy neutralino NLSP of $m_{\tilde \chi} \gtrsim 400$ GeV decaying predominantly to Z-boson plus a light gravitino, such that nearly every gluino produces at least one Z-boson in its decay chain, could reproduce the excess. We construct an explicit general gauge mediation model able to reproduce the observed signal overcoming all the experimental limits. Needless to say, more sophisticated models could also reproduce the signal, however, any model would have to exhibit the following features, light gluinos, or heavy particles with a strong production cross-section, producing at least one Z-boson in its decay chain. The implications of our findings for the Run II at LHC with the scaling on the Z peak, as well as for the direct search of gluinos and other SUSY particles, are pointed out.

https://dx.doi.org/10.48550/arxiv.1503.04184