Bibcode
Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Asilar, E.; Bergauer, T.; Brandstetter, J.; Brondolin, E.; Dragicevic, M.; Erö, J.; Flechl, M.; Friedl, M.; Frühwirth, R.; Ghete, V. M.; Hartl, C.; Hörmann, N.; Hrubec, J.; Jeitler, M.; König, A.; Krätschmer, I.; Liko, D.; Matsushita, T.; Mikulec, I.; Rabady, D.; Rad, N.; Rahbaran, B.; Rohringer, H.; Schieck, J.; Strauss, J.; Treberer-Treberspurg, W.; Waltenberger, W.; Wulz, C.-E.; Mossolov, V.; Shumeiko, N.; Suarez Gonzalez, J.; Alderweireldt, S.; De Wolf, E. A.; Janssen, X.; Lauwers, J.; Van De Klundert, M.; Van Haevermaet, H.; Van Mechelen, P.; Van Remortel, N.; Van Spilbeeck, A.; Abu Zeid, S.; Blekman, F.; D'Hondt, J.; Daci, N.; De Bruyn, I.; Deroover, K.; Heracleous, N.; Lowette, S.; Moortgat, S.; Moreels, L.; Olbrechts, A.; Python, Q.; Tavernier, S.; Van Doninck, W.; Van Mulders, P.; Van Parijs, I.; Brun, H.; Caillol, C.; Clerbaux, B.; De Lentdecker, G.; Delannoy, H.; Fasanella, G.; Favart, L.; Goldouzian, R.; Grebenyuk, A.; Karapostoli, G.; Lenzi, T.; Léonard, A.; Luetic, J.; Maerschalk, T.; Marinov, A.; Randle-conde, A.; Seva, T.; Vander Velde, C.; Vanlaer, P.; Yonamine, R.; Zenoni, F.; Zhang, F.; Cimmino, A.; Cornelis, T.; Dobur, D.; Fagot, A.; Garcia, G.; Gul, M.; Poyraz, D.; Salva, S.; Schöfbeck, R.; Tytgat, M.; Van Driessche, W.; Yazgan, E.; Zaganidis, N.; Bakhshiansohi, H.; Beluffi, C.; Bondu, O.; Brochet, S.; Bruno, G. et al.
Bibliographical reference
Physical Review D, Volume 95, Issue 1, id.012003
Advertised on:
1
2017
Journal
Citations
6
Refereed citations
6
Description
An inclusive search for supersymmetry using razor variables is performed
in events with four or more jets and no more than one lepton. The
results are based on a sample of proton-proton collisions corresponding
to an integrated luminosity of 2.3 fb-1 collected with the
CMS experiment at a center-of-mass energy of √{s }=13 TeV . No
significant excess over the background prediction is observed in data,
and 95% confidence level exclusion limits are placed on the masses of
new heavy particles in a variety of simplified models. Assuming that
pair-produced gluinos decay only via three-body processes involving
third-generation quarks plus a neutralino, and that the neutralino is
the lightest supersymmetric particle with a mass of 200 GeV, gluino
masses below 1.6 TeV are excluded for any branching fractions for the
individual gluino decay modes. For some specific decay mode scenarios,
gluino masses up to 1.65 TeV are excluded. For decays to first- and
second-generation quarks and a neutralino with a mass of 200 GeV,
gluinos with masses up to 1.4 TeV are excluded. Pair production of top
squarks decaying to a top quark and a neutralino with a mass of 100 GeV
is excluded for top squark masses up to 750 GeV.