Cargando…
Probing the Standard Model of particle physics with $t\bar{t}H$, $WWZ$ and $WZZ$ multilepton final states
The Standard Model of particle physics elegantly describes the fundamental constituents of matter and their interactions. The electroweak gauge and top-quark Yukawa couplings can be directly probed in the associated productions of three massive vector bosons and the Higgs boson w...
Autor principal: | |
---|---|
Lenguaje: | eng |
Publicado: |
2019
|
Materias: | |
Acceso en línea: | http://cds.cern.ch/record/2688429 |
Sumario: | The Standard Model of particle physics elegantly describes the fundamental constituents of matter and their interactions. The electroweak gauge and top-quark Yukawa couplings can be directly probed in the associated productions of three massive vector bosons and the Higgs boson with a top-quark pair, respectively. Two dedicated searches in multilepton final states are presented in this dissertation, using data collected in 2015, 2016 and 2017 with the ATLAS detector at the Large Hadron Collider. Both analyses are performed with proton--proton events corresponding to an integrated luminosity of $80\,\text{fb}^{-1}$ at a centre-of-mass energy of $\,\sqrt{s}=13\,\text{TeV}$ and exploit multivariate techniques to discriminate between signal and background processes. A best-fit value of $1.0^{+1.0}_{-0.7}$ is measured for the $t\bar{t}H$ signal strength ${\mu_{t\bar{t}H}=\sigma_{t\bar{t}H}^{\text{obs}}/\sigma_{t\bar{t}H}^{\text{SM}}}$ in the non-resonant four-lepton final state, corresponding to $1.5\sigma$ for the rejection of the no-$t\bar{t}H$ hypothesis. The latest ATLAS $t\bar{t}H$ combination, involving several channels, has provided observation of $t\bar{t}H$ production and, therefore, top-quark Yukawa coupling. The first search for the production of the $WWZ$ and $WZZ$ processes has allowed to reject the background-only hypothesis at the $2.9\sigma$ level. The combination of this analysis with the $WWW$ search provides evidence for the production of three massive vector bosons, rejecting the no-$VVV$ hypothesis at the $4.0\sigma$ level and yielding a best-fit signal strength of ${\mu_{VVV}=1.4\pm0.4}$. |
---|