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Search for a heavy resonance decaying into a Z boson and a vector boson in the \( \nu \overline{\nu}\mathrm{q}\overline{\mathrm{q}} \) final state

(experiments) - boson HJEP07(218)5 and a vector boson in the qq nal state The CMS collaboration 1 Introduction 2 The CMS detector 3 Data and simulated samples 4 Event reconstruction 5 Event selection 6 ... Background estimation 7 Systematic uncertainties 8 Results 9 Summary The CMS collaboration the proposed spin-2 particle and ek = k=M Pl, where k is the curvature parameter of the ve-dimensional space-time

Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at \( \sqrt{s}=13 \) TeV

analysis is based on proton-proton collision data, collected by the CMS Collaboration at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb−1. No significant excess above the standard ... stringent limits on the WR mass to date. Beyond Standard Model; Hadron-Hadron scattering (experiments) - The CMS collaboration 1 Introduction 2 The CMS detector 3 Trigger, particle reconstruction, and

Measurement of normalized differential \( \mathrm{t}\overline{\mathrm{t}} \) cross sections in the dilepton channel from pp collisions at \( \sqrt{s}=13 \) TeV

CMS collaboration 1 Introduction 2 The CMS detector and simulation 2.1 2.2 Signal and background simulation 3 Object and event selection 4 Signal de nition 5 Reconstruction of the tt system 6 Normalized ... CMS collaboration energies of 7 [2, 3] and 8 TeV [4{12]. The dilepton (electron or muon) nal state of the tt decay helps in the suppression of background events. This paper presents the rst CMS s = 13

Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at \( \sqrt{s_{\mathrm{NN}}}=5.02 \) TeV

Introduction 2 3 4 5 6 7 avor subprocess reweighting The CMS collaboration this phenomenon at the LHC was the transverse momentum (pT) balance of back-to-back jets [2{5]. Quenching imparts a net imbalance to

Measurement of differential cross sections in the kinematic angular variable ϕ* for inclusive Z boson production in pp collisions at $$ \sqrt{s}=8 $$ TeV

-Hadron scattering (experiments); Particle correlations and uctua- - boson 8 TeV p The CMS collaboration for < 1. The measurements are compared to theoretical predictions and they agree, typically ... Theoretical predictions 10 Results 11 Summary The CMS collaboration 1 Introduction The neutral current Drell-Yan (DY) process, qq ! Z= ! `+` , where ` is either an electron or a muon, is one of the best

Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at \( \sqrt{s}=8 \) TeV

model of gauge-mediated SUSY breaking that leads to exclusion of top squark masses below 650{730 GeV. Hadron-Hadron scattering (experiments); Supersymmetry - The CMS collaboration 1 Introduction 2 3 ... 4 5 6 Event selection and analysis strategy Results and interpretation Summary The CMS collaboration ing to an integrated luminosity of 19.7 fb 1 of pp collisions at p In this paper, we describe a

Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV

analyses. Hadron-Hadron scattering (experiments); Supersymmetry - The CMS collaboration 1 Introduction 2 Signal models 3 The CMS detector 5 Individual searches 7 Interpretation 8 Summary The CMS ... collaboration 1 Introduction 4 Event reconstruction and Monte Carlo simulation Search for one lepton, two b jets, and pTmiss Search for two leptons consistent with a Z boson, jets, and pTmiss 5.6 Search for a

Measurement of the inclusive $$ \mathrm{t}\overline{\mathrm{t}} $$ cross section in pp collisions at s=5.02$$ \sqrt{s}=5.02 $$ TeV using final states with at least one charged lepton

gluon distribution function is investigated. Hadron-Hadron scattering (experiments); Top physics - 5.02 TeV The CMS collaboration 3 Data, simulated samples and theoretical cross section 1 Introduction ... section 8.1 8.2 The `+jets nal state The dilepton nal state 8.3 Combination 9 QCD analysis 10 Summary The CMS collaboration in proton-proton (pp) collisions have been published at p by the gluon, where

Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $$ \sqrt{s}=13 $$ TeV

scattering (experiments); Supersymmetry; Beyond Standard - 13 TeV HJEP03(218)76 p The CMS collaboration 1 Introduction 2 Signal models 3 The CMS detector 4 Data sets, triggers, and object selection 5 Signal ... assumption of strong SUSY production. Searches for SUSY in these nal states were performed previously by the CMS [13{18] and ATLAS [19{21] Collaborations. The CMS Collaboration reported the presence of an

Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV

, providing a compromise between simplicity and analysis sensitivity. Hadron-Hadron scattering (experiments); Supersymmetry; Lepton produc- - The CMS collaboration 1 Introduction 2 3 4 5 6 7 8 Search ... strategy Background estimation Systematic uncertainties Results Conclusions The CMS collaboration The CMS detector Event selection criteria and Monte Carlo simulation at a center-of-mass energy of 13 TeV

Constraints on the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at $$ \sqrt{s}=8 $$ TeV

4.1 4.2 4.3 4.4 Event selection Background evaluation Multivariate analysis Systematic uncertainties Results Summary The CMS collaboration 2 3 4 5 6 as: 1 Introduction In proton-proton (pp

Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV

presented. The analysis is based on data collected in proton-proton collisions at p Jet substructure; Hadron-Hadron scattering (experiments); Dark matter; Jets - The CMS collaboration s = 13 TeV with the ... selection 3.1 3.2 Simulated samples Event reconstruction and selection 4 Background estimate 5 Systematic uncertainties 6 Results 7 Summary A Supplementary materials The CMS collaboration D0 [20

Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV

Georgian Technical University , Tbilisi , Georgia 16 University , Budapest , Hungary - Erratum The CMS collaboration https://doi.org/10.1007/JHEP01(2018)056 In the original paper, gure 10 was incorrect

Search for anomalous single top quark production in association with a photon in pp collisions at $$ \sqrt{s}=8 $$ TeV

-space region. These are the most stringent limits currently available. Flavour Changing Neutral Currents; Hadron-Hadron scattering (experi- - The CMS collaboration 1 Introduction 2 The CMS detector 3 ... the FCNC cross sections for a restricted phase space 10 Summary The CMS collaboration 1 Introduction predicted branching fraction (B) for t ! u and t ! c decays are approximately 10 14 [ 2 ]. However