Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at √s = 8 TeV
Metadatos
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Springer
Materia
Hadron-Hadron Scattering
Date
2015-07-29Referencia bibliográfica
Aad, G. & Rodríguez Chala, M. & Atlas Collaboration. J. High Energ. Phys. 2015, 162 (2015). [https://doi.org/10.1007/JHEP07(2015)162]
Patrocinador
CERN for the very successful operation of the LHC; ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; RGC, Hong Kong SAR, China; ISF, MINERVA, GIF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW and NCN, Poland; GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MIZˇS, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; R, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America; Crucial computing support from all WLCG partnersRésumé
A search for heavy Majorana neutrinos in events containing a pair of high-pT
leptons of the same charge and high-pT jets is presented. The search uses 20.3 fb−1 of
pp collision data collected with the ATLAS detector at the CERN Large Hadron Collider
with a centre-of-mass energy of √s = 8TeV. The data are found to be consistent with the
background-only hypothesis based on the Standard Model expectation. In the context of
a Type-I seesaw mechanism, limits are set on the production cross-section times branching
ratio for production of heavy Majorana neutrinos in the mass range between 100 and
500 GeV. The limits are subsequently interpreted as limits on the mixing between the
heavy Majorana neutrinos and the Standard Model neutrinos. In the context of a left-right
symmetric model, limits on the production cross-section times branching ratio are set with
respect to the masses of heavy Majorana neutrinos and heavy gauge bosons WR and Z`.