Abstract

An improved measurement of the mass of the Higgs boson is derived from a combined fit to the reconstructed invariant mass spectra of the decay channels H→γγ and H→ZZ*→4ℓ. The analysis uses the pp collision data sample recorded by the ATLAS experiment at the CERN Large Hadron Collider at center-of-mass energies of 7 TeV and 8 TeV, corresponding to an integrated luminosity of 25 fb−1. The measured value of the Higgs boson mass is mH=125.36±0.37(stat)±0.18(syst) GeV. This result is based on improved energy-scale calibrations for photons, electrons, and muons as well as other analysis improvements, and supersedes the previous result from ATLAS. Upper limits on the total width of the Higgs boson are derived from fits to the invariant mass spectra of the H→γγ and H→ZZ*→4ℓ decay channels.2 MoreReceived 17 June 2014DOI:https://doi.org/10.1103/PhysRevD.90.052004This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.© 2014 CERN, for the ATLAS Collaboration

Highlights

  • In 2012, the ATLAS and CMS collaborations published the discovery of a new particle [1,2] in the search for the Standard Model (SM) Higgs boson [3,4,5,6,7,8] at the CERN Large Hadron Collider (LHC) [9]

  • (v) Uncertainty in the modeling of the lateral shower shape: differences between data and simulation for the lateral development of electromagnetic showers contribute to the uncertainty on the energy scale if they depend on energy or particle type

  • The parameters of the functional form used to generate these pseudo-experiments are determined from the data. These pseudo-experiments are fitted using the nominal background model. This procedure leads to an uncertainty on the mass measurement between 0.01% and 0.05% depending on the category, and smaller than the uncertainties derived from the baseline method using the large sample of simulated background events

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Summary

INTRODUCTION

In 2012, the ATLAS and CMS collaborations published the discovery of a new particle [1,2] in the search for the Standard Model (SM) Higgs boson [3,4,5,6,7,8] at the CERN Large Hadron Collider (LHC) [9]. The measurement of the Higgs boson mass is updated in this work with improved analyses of the two channels H → γγ and H → ZZÃ → 4l, as described in Secs. The H → γγ channel profits from an improved calibration of the energy measurements of electron and photon candidates, which results in a sizable reduction of the systematic uncertainties on their energy scales. In the H → ZZÃ → 4l channel both the expected statistical uncertainty and the systematic uncertainty on the mass measurement have been reduced with respect to the previous publication. IV and V a brief description of the analyses used to measure the Higgs boson mass in the H → γγ and H → ZZÃ → 4l channels is presented, with emphasis on the improvements with respect to the analysis published in Ref. The range for electrons from H → ZZÃ → 4l decays is from 7 GeV to about 50 GeV

Definition of photon and electron objects
Cell energy calibration and stability
Intercalibration of the different calorimeter layers
Determination of the material in front of the EM calorimeter
Global calorimeter energy scale adjustment
Systematic uncertainties on the energy scale and cross-checks
Uncertainties on the calorimeter energy resolution
Event selection
Event categorization
Signal modeling
Background modeling and estimation
Mass measurement method
Systematic uncertainties
Result
Background estimation
Multivariate discriminant
Signal and background model
Results
Background
STATISTICAL PROCEDURE AND TREATMENT OF SYSTEMATIC UNCERTAINTIES
COMBINED MASS MEASUREMENT
Findings
VIII. CONCLUSIONS
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