Abstract
A study of the $CP$ properties of the interaction between the Higgs boson and top quarks is presented. Higgs bosons are identified via the diphoton decay channel ($H \rightarrow \gamma\gamma$) and their production in association with a top quark pair ($t\bar{t}H$) or single top quark ($tH$) is studied. The analysis uses 139 fb$^{-1}$ of proton-proton collision data recorded at a center-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS detector at the Large Hadron Collider. Assuming a $CP$-even coupling, the $t\bar{t}H$ process is observed with a significance of 5.2 standard deviations. The measured cross section times $H \to \gamma \gamma$ branching ratio is $1.64\;^{+0.38}_{-0.36}\;\text{(stat.)}\;^{+0.17}_{-0.14}\;(\text{sys.})$ fb, and the measured rate for $t\bar{t}H$ is $1.43\;^{+0.33}_{-0.31}\;\text{(stat.)}\;^{+0.21}_{-0.15}\;(\text{sys.})$ times the Standard Model expectation. The $tH$ production process is not observed and an upper limit on its rate of 12 times the Standard Model expectation is set. A $CP$-mixing angle greater (less) than 43 (-43)$^\circ$ is excluded at 95% confidence level.
Highlights
The effective field theory (EFT) definition used in this Letter is provided by theHiggs characterization model [21], which is implemented in the MADGRAPH5_AMC@NLO generator [22]
A study of the charge conjugation and parity (CP) properties of the interaction between the Higgs boson and top quarks is presented
Studies of CP properties of the Higgs boson interactions with gauge bosons have been performed by the ATLAS and CMS experiments [4,5,6,7,8,9]; the results show no deviations from the Standard Model (SM) predictions
Summary
Higgs characterization model [21], which is implemented in the MADGRAPH5_AMC@NLO generator [22]. This model, the term in the effective Lagrangian that describes the top Yukawa coupling is. Mt v fψtκt1⁄2cosðαÞ þ i sinðαÞγ5ψ tgH where mt is the top quark mass, v is the Higgs vacuum expectation value, κt (> 0) is the top Yukawa coupling parameter, and α is the CP-mixing angle.
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