Abstract

Inclusive and differential fiducial cross sections of Higgs boson production in proton-proton collisions are measured in the H → ZZ* → 4ℓ decay channel. The proton-proton collision data were produced at the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector in 2015 and 2016, corresponding to an integrated luminosity of 36.1 fb−1. The inclusive fiducial cross section in the H → ZZ* → 4ℓ decay channel is measured to be 3.62 ± 0.50(stat)− 0.20+ 0.25 (sys) fb, in agreement with the Standard Model prediction of 2.91 ± 0.13 fb. The cross section is also extrapolated to the total phase space including all Standard Model Higgs boson decays. Several differential fiducial cross sections are measured for observables sensitive to the Higgs boson production and decay, including kinematic distributions of jets produced in association with the Higgs boson. Good agreement is found between data and Standard Model predictions. The results are used to put constraints on anomalous Higgs boson interactions with Standard Model particles, using the pseudo-observable extension to the kappa-framework.

Highlights

  • ZZ* Background Z+jets, tt, tt+V, VVV Uncertainty mF4lSR-corrected [GeV]highest expected signal rate after reconstruction and event selection is selected, in the order: 4μ, 2e2μ, 2μ2e and 4e

  • Inclusive and differential fiducial cross sections of Higgs boson production in proton-proton collisions are measured in the H → ZZ∗ → 4 decay channel

  • Several differential fiducial cross sections are measured for observables sensitive to the Higgs boson production and decay, including kinematic distributions of jets produced in association with the Higgs boson

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Summary

ATLAS detector

The ATLAS detector [17] is a multi-purpose detector with a forward-backward symmetric cylindrical geometry. The inner detector (ID), immersed in a 2 T magnetic field produced by a thin superconducting solenoid located in front of the calorimeter, 1ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point (IP) in the centre of the detector and the z-axis along the beam pipe. The silicon-based detectors cover the pseudorapidity range |η| < 2.5. A liquid-argon calorimeter with copper absorbers is used in the hadronic endcap calorimeters, which covers the region 1.5 < |η| < 3.2. A forward calorimeter using copper or tungsten absorbers with liquid argon completes the calorimeter coverage up to |η| = 4.9. Events are selected using a first-level trigger implemented in custom electronics, which reduces the event rate to a maximum of 100 kHz using a subset of detector information. Software algorithms with access to the full detector information are used in the high-level trigger to yield a recorded event rate of about 1 kHz [20]

Theoretical predictions and event simulation
Event selection
Background
Fiducial phase space
Background estimates
Measured data yields
Signal extraction and correction for detector effects
ATLAS Simulation
Systematic uncertainties
10 Results
11 Conclusion
Full Text
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