Abstract

The properties of a Higgs boson candidate are measured in the H to ZZ to 4l decay channel, with l = e, mu, using data from pp collisions corresponding to an integrated luminosity of 5.1 inverse femtobarns at the center-of-mass energy of sqrt(s) = 7 TeV and 19.7 inverse femtobarns at sqrt(s) = 8 TeV, recorded with the CMS detector at the LHC. The new boson is observed as a narrow resonance with a local significance of 6.8 standard deviations, a measured mass of 125.6 +- 0.4 (stat) +- 0.2 (syst) GeV, and a total width less than 3.4 GeV at the 95% confidence level. The production cross section of the new boson times its branching fraction to four leptons is measured to be 0.93 +0.26 -0.23 (stat) +0.13 -0.09 (syst) times that predicted by the standard model. Its spin-parity properties are found to be consistent with the expectations for the standard model Higgs boson. The hypotheses of a pseudoscalar and all tested spin-one boson hypotheses are excluded at the 99% confidence level or higher. All tested spin-two boson hypotheses are excluded at the 95% confidence level or higher.

Highlights

  • The standard model (SM) of particle physics [1,2,3,4,5]describes very successfully the electroweak and strong interactions of elementary particles over a wide range of energies

  • The energy of the electromagnetic calorimeter (ECAL) superclusters is corrected for the imperfect containment of the clustering algorithm, the electron energy not deposited in the ECAL, and leakage arising from showers near gaps between crystals or between ECAL modules

  • The irreducible four-lepton background arising from double-parton interactions (DPI), Z þ Drell-Yan (DY), is evaluated using PYTHIA 6.4.24 with the overall cross section calculated as σDPI 1⁄4 σZ · σDY=σpheno, where the pphffieffi nomenological effective cross section, measured at s 1⁄4 7 TeV, is σpheno 1⁄4 15 mb [107], and the cross sections σZ and σDY are taken from simulation

Read more

Summary

INTRODUCTION

Describes very successfully the electroweak and strong interactions of elementary particles over a wide range of energies. Using 2011 about 5 fb−1 and about 5 of data fb−1 of apdffidffi itional data collected in the first half of 2012 at s 1⁄4 8 TeV, the ATLAS and CMS experiments have reported the discovery of a new boson at a mass around. The analysis of the H → ZZ → 4l channel is presented using the entire data set collected by the CMS experiment during the 2011–2012 LHC running period. A search is conducted for additional resonances compatible with the SM Higgs boson in the H → ZZ → 4l channel in the mass range 110–1000 GeV.

THE CMS DETECTOR
SIMULATED DATA SAMPLES
ONLINE EVENT SELECTION
LEPTON RECONSTRUCTION AND SELECTION
Electron reconstruction and identification
Muon reconstruction and identification
Lepton isolation and vertex compatibility
GeV where and jηj i runs
FINAL-STATE RADIATION RECOVERY
JET RECONSTRUCTION AND IDENTIFICATION
VIII. SELECTION AND CATEGORIZATION OF FOUR-LEPTON CANDIDATES
Per-event mass uncertainties
BACKGROUND
Irreducible background
Reducible background
N2P2F i
N2P2LSS
Combination of the two methods
KINEMATIC DISCRIMINANTS
YIELDS AND KINEMATIC DISTRIBUTIONS
HIGGS BOSON PROPERTIES MEASUREMENT
Multidimensional likelihoods
Systematic uncertainties
XIII. RESULTS AND INTERPRETATION
Signal significance and exclusion limits
Mass and width
H ZZ 4e H ZZ 2e2 H ZZ 4
Spin and parity
CMS 8 7 6
SUMMARY
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call