2015/03/13 by V. Khachatryan, CMS Collaboration, A. M. Sirunyan +98 · 1 voice · 2 citations
Physics and Astronomy · #Astrophysics #Boson #Bottom quark #Gauge (firearms) #Graviton #Higgs boson #High-Energy Particle Collisions Research #Inverse #Large Hadron Collider #Luminosity #Nuclear physics #Pair production #Particle physics #Particle physics theoretical and experimental studies #Physics #Production (economics) #Quantum Chromodynamics and Particle Interactions #Quark #Resonance (particle physics) #Standard Model (mathematical formulation) #Top quark #hep-ex
paper · pdf · doi:10.1016/j.physletb.2015.08.047
published as Phys. Lett. B 749 (2015) 560 · Replaced with published version. Added journal reference and DOI
arxiv published 2015/03/13 · openalex publication_date 2015/08/24 · arxiv created 2015/09/14 · arxiv updated 2015/09/14 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/06
A model-independent search for a narrow resonance produced in proton–proton collisions at s=8TeV and decaying to a pair of 125 GeV Higgs bosons that in turn each decays into a bottom quark–antiquark pair is performed by the CMS experiment at the LHC. The analyzed data correspond to an integrated luminosity of 17.9 fb−1. No evidence for a signal is observed. Upper limits at a 95% confidence level on the production cross section for such a resonance, in the mass range from 270 to 1100 GeV, are reported. Using these results, a radion with decay constant of 1 TeV and mass from 300 to 1100 GeV, and a Kaluza–Klein graviton with mass from 380 to 830 GeV are excluded at a 95% confidence level.