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Published October 13, 2017 | Submitted + Published
Journal Article Open

Search for Supersymmetry in pp Collisions at √s = 13  TeV in the Single-Lepton Final State Using the Sum of Masses of Large-Radius Jets


Results are reported from a search for supersymmetric particles in proton-proton collisions in the final state with a single lepton, multiple jets, including at least one b-tagged jet, and large missing transverse momentum. The search uses a sample of proton-proton collision data at √s = 13  TeV recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9  fb^(−1). The observed event yields in the signal regions are consistent with those expected from standard model backgrounds. The results are interpreted in the context of simplified models of supersymmetry involving gluino pair production, with gluino decay into either on- or off-mass-shell top squarks. Assuming that the top squarks decay into a top quark plus a stable, weakly interacting neutralino, scenarios with gluino masses up to about 1.9 TeV are excluded at 95% confidence level for neutralino masses up to about 1 TeV.

Additional Information

© 2017 CERN, for the CMS Collaboration. Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Received 12 May 2017; published 13 October 2017. We congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centers and personnel of the Worldwide LHC Computing Grid for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC and the CMS detector provided by the following funding agencies: BMWFW and FWF (Austria), FNRS and FWO (Belgium), CNPq, CAPES, FAPERJ, and FAPESP (Brazil), MES (Bulgaria), Conseil Européen pour la Recherche Nucléaire (CERN, Switzerland), CAS, MoST, and NSFC (China), COLCIENCIAS (Colombia), MSES and CSF (Croatia), RPF (Cyprus), SENESCYT (Ecuador), MoER, ERC IUT, and European Regional Development Fund ERDF (Estonia). Academy of Finland, MEC, and Helsinki Institute of Physics (HIP, Finland), CEA and CNRS/IN2P3 (France), BMBF, DFG, and HGF (Germany), GSRT (Greece), OTKA and NIH (Hungary), DAE and DST (India), IPM (Iran), SFI (Ireland), INFN (Italy), MSIP and NRF (Republic of Korea), LAS (Lithuania), Malaysia MOE and UM (Malaysia), BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico), MBIE (New Zealand), PAEC (Pakistan), MSHE and NSC (Poland), FCT (Portugal), JINR (Dubna), MON, RosAtom, RAS, RFBR, and RAEP (Russia), MESTD (Serbia), SEIDI and CPAN (Spain), Swiss Funding Agencies (Switzerland), Ministry of Science and Technology (MST Taipei), Thailand Center of Excellence in Physics (ThEPCenter), Institute for the Promotion of Teaching Science and Technology of Thailand (IPST), Special Task Force for Activating Research (STAR), and NSTDA (Thailand), TUBITAK and TAEK (Turkey), NASU and SFFR (Ukraine), STFC (United Kingdom), DOE and NSF (U.S.).

Attached Files

Published - PhysRevLett.119.151802.pdf

Submitted - 1605.04608.pdf


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August 19, 2023
October 17, 2023