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Search for top-antitop quark resonances with the ATLAS detector at the Large Hadron Collider
The intriguing nature of the top quark, by far the heaviest particle in the Standard Model of particle physics, has motivated the development of many theoretical extensions predicting the existence of new massive particles decaying to a pair of top-antitop quarks. The production of these hypothetica...
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Lenguaje: | eng |
Publicado: |
2018
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/2318411 |
Sumario: | The intriguing nature of the top quark, by far the heaviest particle in the Standard
Model of particle physics, has motivated the development of many theoretical
extensions predicting the existence of new massive particles decaying to a pair of
top-antitop quarks. The production of these hypothetical particles in proton-proton
collisions at the Large Hadron Collider would reveal itself as a resonance in the
expected smooth distribution of the top-antitop quark invariant mass. This thesis
presents a search for such a new heavy particle decaying to a pair of top-antitop
quarks in the semi-leptonic final state. The analyzed data sample amounts to a
total of 4.6 fb−1 at a proton-proton collision center-of-mass energy of 7 TeV. Novel
techniques specifically tailored to the identification of the decay products of highly
energetic top quarks are developed and used. No evidence for resonant production
of pairs of top-antitop quarks is found and, as a result, constraints are set on two
theoretical models. Upper limits on the production cross-section times branching
ratio are established at a 95% credibility level for a leptophobic Z
′ boson from the
Topcolor model, and a Kaluza-Klein gluon from the Randall-Sundrum model. The
Z
′ boson and the Kaluza-Klein gluon are excluded to exist (at a 95% credibility level)
in the mass ranges 0.8-1.65 TeV and 0.8-1.88 TeV, respectively. The constraints derived
in this thesis on the two theoretical models are more stringent than the ones
obtained at other experiments, thanks to the large center-of-mass energy and the
dedicated high-energy top quark identification techniques used. |
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