Search for an invisible scalar in $t \bar{t}$ final states at the LHC
Duarte Azevedo, Rodrigo Capucha, Pedro Chaves, Jo\~ao Bravo Martins,, Ant\'onio Onofre, Rui Santos

TL;DR
This study searches for an invisible scalar mediator in top-antitop events at the LHC, using a phenomenological approach to reconstruct the system and probe CP properties, setting limits on couplings across various mediator masses.
Contribution
It introduces a method to reconstruct $tar{t}$ systems with a scalar mediator and uses CP angular observables to constrain mediator-top couplings at the LHC.
Findings
Reconstructed $tar{t}$ system with a scalar mediator using kinematic fit.
Set confidence level limits on Yukawa couplings as a function of mediator mass.
Analyzed CP properties of the mediator-top coupling.
Abstract
We use the current experimental analysis to look for Dark Matter (DM) particles hidden in the final state. We present a phenomenological study where we successfully perform the reconstruction of a system in the presence of a scalar mediator , that couples to both Standard Model (SM) and to DM particles. We use a \texttt{MadGraph5\_aMC@NLO} simplified DM model, where signal samples of are generated at the Large Hadron Collider (LHC) with both Charge-Parity (CP) -even and CP-odd couplings of to the top quarks. Different mass scales for the mediator are considered, from the low mass region ( 0~GeV) to masses close to the Higgs boson mass (125~GeV). The dileptonic final states of the system were used in our analysis. The reconstruction of the system is done with a kinematic fit, without…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsParticle physics theoretical and experimental studies · Dark Matter and Cosmic Phenomena · Particle Detector Development and Performance
