Abstract
We explore the direct Higgs boson-top $CP$ measurement via the $pp\ensuremath{\rightarrow}t\overline{t}h$ channel at the high-luminosity LHC. We show that a combination of machine learning techniques and efficient kinematic reconstruction methods can boost new physics sensitivity, effectively probing the complex $t\overline{t}h$ multiparticle phase space. Special attention is devoted to top quark polarization observables, uplifting the analysis from a raw rate to a polarization study. Through a combination of hadronic, semileptonic, and dileptonic top pair final states in association with $h\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma}$, we obtain that the HL-LHC can probe the Higgs boson-top coupling modifier and $CP$ phase, respectively, up to $|{\ensuremath{\kappa}}_{t}|\ensuremath{\lesssim}8%$ and $|\ensuremath{\alpha}|\ensuremath{\lesssim}13\ifmmode^\circ\else\textdegree\fi{}$ at 68% C.L.
Highlights
New sources of CP violation can be a key ingredient to explain the matter-antimatter asymmetry of the Universe [1,2,3]
We show that a combination of machine learning techniques and efficient kinematic reconstruction methods can boost new physics sensitivity, effectively probing the complex tth multiparticle phase space
We show that the ability of probing the pp → tth channel exploring the complex multiparticle final state in terms of a raw rate, but as a polarized process, can offer a crucial pathway to probe the underlying production dynamics, accessing possible new physics effects
Summary
New sources of CP violation can be a key ingredient to explain the matter-antimatter asymmetry of the Universe [1,2,3]. Whereas it is possible to access the Higgs boson-top coupling through loop induced processes [7,8,9,10,11,12,13,14], the direct Higgs boson-top production via pp → tth is crucial to disentangle possible new physics effects [6,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32] This channel was observed in 2018 by both ATLAS and CMS with significances of 6.3 and 5.2σ, respectively [25,26].
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