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Evidence for the direct decay of the 125 GeV Higgs boson to fermions

). Recently, the CMS Collaboration reported on a search for the decays of the new boson to quark pairs15 as well as to ττ lepton pairs16 based on data collected in 2011 and 2012. In this Letter, we report on ... standard model expectation for a Higgs boson in the 110–130 GeV mass range23,24. Evidence for a Higgs boson decaying to a ττ lepton pair is reported by the CMS Collaboration in ref. 16. The lifetime of the

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