Neutralino dark matter confronted by the LHC constraints on electroweak SUSY signals

被引:26
作者
Choudhury A. [1 ]
Datta A. [1 ]
机构
[1] Indian Institute of Science Education and Research - Kolkata, Mohanpur Campus, PO, BCKV Campus Main Office, Nadia
关键词
Supersymmetry Phenomenology;
D O I
10.1007/JHEP09(2013)119
中图分类号
学科分类号
摘要
The supersymmetric particles (sparticles) belonging exclusively to the electroweak sector of the minimal supersymmetric standard model (MSSM) may hold the key to the observed dark matter relic density in the universe even if all strongly interacting sparticles are very heavy. The importance of the light EW sparticles in DM physics and in producing spectacular collider signals is emphasized. It is shown that even the preliminary data on the direct searches of these sparticles at the LHC, significantly constrain the parameter space of the MSSM compatible with the observed relic density and provide useful hints about the future search prospects. If in addition to the electroweak sparticles the gluinos are also within the reach of the LHC experiments, then the gluino mass limits in the light slepton scenario obtained via the canonical jets + Slashed E signT channel may be relaxed by as much as 25% compared to the existing limits. But the corresponding same sign dilepton (SSD) + jets + Slashed E signT signal will yield enhanced limits competitive with the strongest limits currently available. This is illustrated with the help of benchmark scenarios at the generator level using PYTHIA. If the gluinos are just beyond the current reach of the LHC, then the generic n-lepton + m-jets + missing energy signal may discriminate between different DM producing mechanisms by comparing the signals corresponding to different values of n. This is illustrated by simulating the signals for n = 0 and n = 2 (the SSD signal). © SISSA 2013.
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[11]  
Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb<sup>-1</sup> of √s = 7 TeV proton-proton collision data, Phys. Rev. D, 87, (2013)
[12]  
of √S = 8 TeV Proton-proton Collisions, (2012)
[13]  
Search for Supersymmetry at √S = 8 TeV in Final States with Jets, Missing Transverse Momentum and One Isolated Lepton, (2012)
[14]  
Search for new physics in events with same-sign dileptons and b jets in pp collisions at √s = 8 TeV, JHEP, 3, (2013)
[15]  
Inclusive search for supersymmetry using the razor variables in pp collisions at √s = 7 TeV, Phys. Rev. Lett., 111, (2013)
[16]  
and B-quark Multiplicity in Pp Collisions at √S = 8 TeV
[17]  
of √S = 8TeV Proton-proton Collision Data, (2012)
[18]  
Search for Supersymmetry in Final States with Two Same-sign Leptons, Jets and Missing Transverse Momentum with the ATLAS Detector in Pp Collisions at √S = 8 TeV, (2012)
[19]  
Bechtle P., Et al., What if the LHC does not find supersymmetry in the √s = 7 TeV run?, Phys. Rev. D, 84, (2011)
[20]  
Akula S., Et al., Interpreting the first CMS and ATLAS SUSY results, Phys. Lett. B, 699, (2011)