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Measurement of the $t\bar{t}H$ Production Cross-Section in the Non-Resonant Four Lepton Final State in $pp$ Collisions at $\sqrt{s}=13\,\text{TeV}$ with the ATLAS Detector

dc.contributor.advisorQuadt, Arnulf Prof. Dr.
dc.contributor.authorEggebrecht, Stephen
dc.date.accessioned2025-11-26T18:41:24Z
dc.date.available2025-12-03T00:50:06Z
dc.date.issued2025-11-26
dc.identifier.urihttp://resolver.sub.uni-goettingen.de/purl?ediss-11858/16367
dc.identifier.urihttp://dx.doi.org/10.53846/goediss-11659
dc.format.extent209de
dc.language.isoengde
dc.subject.ddc530de
dc.titleMeasurement of the $t\bar{t}H$ Production Cross-Section in the Non-Resonant Four Lepton Final State in $pp$ Collisions at $\sqrt{s}=13\,\text{TeV}$ with the ATLAS Detectorde
dc.typedoctoralThesisde
dc.contributor.refereeQuadt, Arnulf Prof. Dr.
dc.date.examination2025-02-03de
dc.subject.gokPhysik (PPN621336750)de
dc.description.abstractengThis thesis presents the measurements of the associated production of a top quark pair with a Standard Model Higgs boson in multi-lepton final states, focusing on the measurement of the inclusive cross-section in the $4\ell$ channel. The analysis uses the full Run 2 data set, corresponding to an integrated luminosity of $140\,\text{fb}^{-1}$, collected in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\,\text{TeV}$. The analysis covers six final states, defined by the number and flavour of charged-lepton candidates. Machine learning techniques are used for all channels to improve signal sensitivity. Leading prompt background contributions from $t\bar{t}Z$, $t\bar{t}W$, and diboson production are constrained by additional regions populated with those backgrounds. Moreover, contributions from fake and non-prompt leptons are estimated using data-driven methods such as the fake factor or template method. The observed signal strength, the ratio of the measured signal yield over the Standard Model prediction, is extracted using a profile likelihood fit. For the $4\ell$ channel, the observed signal strength is $\mu_{t\bar{t}H}=0.53^{+0.67}_{-0.53}=0.53^{+0.66}_{-0.51}\left(\text{stat.}\right)^{+0.13}_{-0.13}\left(\text{sys.}\right)$, corresponding to an observed (expected) significance of $0.95\sigma$ ($1.80\sigma$). The measured signal strength for the combination of all six channels is $\mu_{t\bar{t}H}=0.63^{+0.20}_{-0.19}=0.63^{+0.17}_{-0.16}\left(\text{stat.}\right)^{+0.11}_{-0.10}\left(\text{sys.}\right)$. It corresponds to an observed (expected) significance of $3.3\sigma$ ($5.3\sigma$). The measured inclusive cross-section is found to be $321^{+102}_{-99}\,\text{fb}$. The compatibility is $7.2\,\%$ with the Standard Model prediction of $507^{+35}_{-50}\,\text{fb}$. The signal strength is also measured in bins of the Higgs boson transverse momentum and demonstrates a compatibility of $28\,\%$ with the Standard Model prediction.de
dc.contributor.coRefereeDéliot, Frédéric Dr.
dc.subject.engExperimental Particle Physicsde
dc.subject.engATLASde
dc.subject.engLHCde
dc.subject.engCERNde
dc.subject.engHiggs Bosonde
dc.subject.engTop Quarkde
dc.subject.engttHde
dc.subject.engYukawa Couplingde
dc.subject.engMachine Learningde
dc.subject.engMultileptonde
dc.subject.engFake Estimationde
dc.identifier.urnurn:nbn:de:gbv:7-ediss-16367-5
dc.affiliation.instituteFakultät für Physikde
dc.description.embargoed2025-12-03de
dc.identifier.ppn1942652054
dc.notes.confirmationsentConfirmation sent 2025-11-26T19:45:01de


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