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@ARTICLE{Sirunyan:402418,
author = {Sirunyan, A. M. and others},
collaboration = {{CMS Collaboration}},
title = {{S}earch for supersymmetry in events with one lepton and
multiple jets exploiting the angular correlation between the
lepton and the missing transverse momentum in proton-proton
collisions at $\sqrt{s} = $ 13 {T}e{V}},
journal = {Physics letters / B},
volume = {780},
issn = {0370-2693},
address = {Amsterdam},
publisher = {North-Holland Publ.},
reportid = {PUBDB-2018-01834, CMS-SUS-16-042. CERN-EP-2017-201.
arXiv:1709.09814},
pages = {384 - 409},
year = {2018},
note = {All the figures and tables, including additional
supplementary figures and tables, can be found at
http://cms-results.web.cern.ch/cms-results/public-results/publications/SUS-16-042/
(CMS Public Pages)},
abstract = {Results are presented from a search for supersymmetry in
events with a single electron or muon and hadronic jets. The
data correspond to a sample of proton–proton collisions at
$\sqrt{s}$=13TeV with an integrated luminosity of 35.9
fb$^{−1}$ , recorded in 2016 by the CMS experiment. A
number of exclusive search regions are defined according to
the number of jets, the number of b -tagged jets, the scalar
sum of the transverse momenta of the jets, and the scalar
sum of the missing transverse momentum and the transverse
momentum of the lepton. Standard model background events are
reduced significantly by requiring a large azimuthal angle
between the direction of the lepton and of the reconstructed
W boson, computed under the hypothesis that all of the
missing transverse momentum in the event arises from a
neutrino produced in the leptonic decay of the W boson. The
numbers of observed events are consistent with the
expectations from standard model processes, and the results
are used to set lower limits on supersymmetric particle
masses in the context of two simplified models of gluino
pair production. In the first model, where each gluino
decays to a top quark–antiquark pair and a neutralino,
gluino masses up to 1.8 TeV are excluded at the 95\% CL. The
second model considers a three-body decay to a light
quark–antiquark pair and a chargino, which subsequently
decays to a W boson and a neutralino. In this model, gluinos
are excluded up to 1.9 TeV.},
keywords = {p p: colliding beams (INSPIRE) / transverse momentum:
missing-energy (INSPIRE) / p p: scattering (INSPIRE) / jet:
transverse momentum (INSPIRE) / lepton: transverse momentum
(INSPIRE) / gluino: decay (INSPIRE) / jet: multiplicity
(INSPIRE) / jet: bottom (INSPIRE) / bottom: particle
identification (INSPIRE) / gluino: mass: lower limit
(INSPIRE) / gluino: pair production (INSPIRE) / W: leptonic
decay (INSPIRE) / final state: ((n)jet lepton) (INSPIRE) /
sparticle: mass: lower limit (INSPIRE) / supersymmetry:
parameter space (INSPIRE) / neutralino (INSPIRE) / angular
correlation (INSPIRE) / background (INSPIRE) / chargino
(INSPIRE) / CERN LHC Coll (INSPIRE) / CMS (INSPIRE) /
experimental results (INSPIRE) / 13000 GeV-cms (INSPIRE)},
cin = {CMS},
ddc = {530},
cid = {I:(DE-H253)CMS-20120731},
pnm = {611 - Fundamental Particles and Forces (POF3-611) /
AMVA4NewPhysics - Advanced Multi-Variate Analysis for New
Physics Searches at the LHC (675440)},
pid = {G:(DE-HGF)POF3-611 / G:(EU-Grant)675440},
experiment = {EXP:(DE-H253)LHC-Exp-CMS-20150101},
typ = {PUB:(DE-HGF)29 / PUB:(DE-HGF)16},
eprint = {1709.09814},
howpublished = {arXiv:1709.09814},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:1709.09814;\%\%$},
UT = {WOS:000432187800059},
doi = {10.1016/j.physletb.2018.03.028},
url = {https://bib-pubdb1.desy.de/record/402418},
}