Abstract

Results are presented for an extraction of the top quark Yukawa coupling from top quark-antiquark ($\mathrm{t\bar{t}}$) kinematic distributions in the lepton plus jets final state in proton-proton collisions, based on data collected by the CMS experiment at the LHC at $\sqrt{s} =$ 13 TeV, corresponding to an integrated luminosity of 35.8 fb$^{-1}$. Corrections from weak boson exchange, including Higgs bosons, between the top quarks can produce large distortions of differential distributions near the energy threshold of $\mathrm{t\bar{t}}$ production. Therefore, precise measurements of these distributions are sensitive to the Yukawa coupling. Top quark events are reconstructed with at least three jets in the final state, and a novel technique is introduced to reconstruct the $\mathrm{t\bar{t}}$ system for events with one missing jet. This technique enhances the experimental sensitivity in the low invariant mass region, $M_\mathrm{t\bar{t}}$. The data yields in $M_\mathrm{t\bar{t}}$, the rapidity difference $|y_\mathrm{t}-y_{\mathrm{\bar{t}}}|$, and the number of reconstructed jets are compared with distributions representing different Yukawa couplings. These comparisons are used to measure the ratio of the top quark Yukawa coupling to its standard model predicted value to be 1.07 $^{+0.34}_{-0.43}$ with an upper limit of 1.67 at the 95% confidence level.

Highlights

  • The study of the properties of the Higgs boson, which is responsible for electroweak symmetry breaking, is one of the main goals of the LHC program

  • Where sbin is the POWHEG prediction for the number of signal tt events; bbin is the prediction for the number of events from all background process; RbinðYt; θÞ 1⁄4 sbinðYtÞ=sbinðPOWHEGÞ encodes the effect of different Yt coupling scenarios, parametrized with a quadratic dependence on Yt in each bin; and θ represents the full suite of nuisance parameters with ρðθÞ described by lognormal distributions parametrizing the uncertainty on each source

  • The tt production cross section is sensitive to the top quark Yukawa coupling through weak force corrections that can modify the distributions of the mass of top quark–antiquark pairs, Mtt, and the rapidity difference between top quark and antiquark, Δytt

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Summary

INTRODUCTION

The study of the properties of the Higgs boson, which is responsible for electroweak symmetry breaking, is one of the main goals of the LHC program. A detailed study of the differential tt kinematic properties close to the production threshold could, determine the value of the top quark Yukawa coupling. When one W boson decays leptonically and the other decays hadronically, tt → WþbW−b → lþνbqq 0bþ charge conjugate, the final state at leading order (LO) consists of an isolated lepton (electron or muon in this analysis), missing transverse momentum (from the neutrino), and four jets (from two b quarks and two light quarks) This final state has a sizable branching fraction of 34%, low backgrounds, and allows for the kinematic reconstruction of the original top quark candidates.

WEAK INTERACTION CORRECTIONS TO tt PRODUCTION
THE CMS DETECTOR
DATA SET AND MODELING
EVENT RECONSTRUCTION AND SELECTION
RECONSTRUCTION OF THE TOP QUARK-ANTIQUARK SYSTEM
Reconstruction of events with at least four jets
Reconstruction of events with exactly three jets
CMS Simulation
BACKGROUND
VIII. EVENT YIELDS AND CONTROL PLOTS
DETERMINATION OF Yt
SYSTEMATIC UNCERTAINTIES
1.25 Simulation
RESULTS
SUMMARY
Methods
Full Text
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