Abstract

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.

Highlights

  • Within this scenario, the ATLAS Collaboration has recently presented an intriguing excess at the 3 sigma level of e+e− and μ+μ− pairs just at the Z peak [9,10], accompanied by hadronic activity and missing transverse energy (MET)

  • By trying to explain this signal with SUSY we find that only relatively light gluinos, mg 1.2 TeV, together with a heavy neutralino NLSP of mχ 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

  • The ATLAS experiment announced a 3 σ excess at the Z -peak consistent of 29 pairs of leptons observed to be compared with 10.6 ± 3.2 expected lepton pairs

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Summary

Introduction

The ATLAS Collaboration has recently presented an intriguing excess at the 3 sigma level of e+e− and μ+μ− pairs just at the Z peak [9,10], accompanied by hadronic activity and missing transverse energy (MET). The observed signal can only be explained if one has a large production cross section of heavy SUSY particles (gluinos or squarks) whose decay chain contains about one Z -boson per parent particle. If such an explanation is the answer to the observed excess, our study points out the way to confirm it in the Run II of LHC, as well as cosmological implications, in particular the particle content of dark matter in the universe.

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Z-boson production in the MSSM
Production cross section of MSSM particles
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Decay of supersymmetric particles to Z -bosons
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G m 2Gm 2χ
A possible explanation in general gauge mediation
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Prospects for SUSY at LHC13
Conclusions
Findings
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Full Text
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