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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

Measurement of inclusive and differential Higgs boson production cross sections in the diphoton decay channel in proton-proton collisions at \( \sqrt{s}=13 \) TeV

Abstract Measurements of the inclusive and differential production cross sections for the Higgs boson in the diphoton decay channel are performed using the data set of proton-proton collisions at \( \sqrt{s}=13 \) TeV collected by the CMS experiment at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb−1. The cross sections are measured in a fiducial phase...

Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at \( \sqrt{s}=13 \) TeV

Abstract Measurements of Higgs boson properties in the H → γγ decay channel are reported. The analysis is based on data collected by the CMS experiment in proton-proton collisions at \( \sqrt{s}=13 \) TeV during the 2016 LHC running period, corresponding to an integrated luminosity of 35.9 fb−1. Allowing the Higgs mass to float, the measurement yields a signal strength relative...

Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at \( \sqrt{s}=13 \) TeV

Abstract A search has been performed for heavy resonances decaying to ZZ or ZW in 2ℓ2q final states, with two charged leptons (ℓ = e, μ) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved...

Search for beyond the standard model Higgs bosons decaying into a \( \mathrm{b}\overline{\mathrm{b}} \) pair in pp collisions at \( \sqrt{s}=13 \) TeV

Abstract A search for Higgs bosons that decay into a bottom quark-antiquark pair and are accompanied by at least one additional bottom quark is performed with the CMS detector. The data analyzed were recorded in proton-proton collisions at a centre-of-mass energy of \( \sqrt{s}=13 \) TeV at the LHC, corresponding to an integrated luminosity of 35.7 fb−1. The final state...

Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at \( \sqrt{s}=13 \) TeV

Abstract A search is presented for long-lived charged particles that decay within the CMS detector and produce the signature of a disappearing track. A disappearing track is an isolated track with missing hits in the outer layers of the silicon tracker, little or no energy in associated calorimeter deposits, and no associated hits in the muon detectors. This search uses data...

Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at \( \sqrt{s}=13 \) TeV

Abstract A measurement is performed of the cross section of top quark pair production in association with a W or Z boson using proton-proton collisions at a center-of-mass energy of 13 TeV at the LHC. The data sample corresponds to an integrated luminosity of 35.9 fb−1, collected by the CMS experiment in 2016. The measurement is performed in the same-sign dilepton, three- and...

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

Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at \( \sqrt{s}=13 \) TeV

energies of 1.96 and 7 TeV respectively. Hadron-Hadron scattering (experiments); Minimum bias; Event-by-event - The CMS collaboration 1 Introduction 2 3 4 5 6 7 Unfolding and systematic uncertainties ... Results and discussion Summary The CMS collaboration 1 Introduction nal-state radiation (FSR), and beambeam remnant (BBR) interactions. The large parton densities accessible in proton-proton (pp

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

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

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

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