A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb −1 of pp collision data collected by the ATLAS detector

This paper presents a search for top-squark pair production in final states with a top quark, a charm quark and missing transverse momentum. The data were collected with the ATLAS detector during LHC Run 2 and correspond to an integrated luminosity of 139 fb −1 of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. The analysis is motivated by an extended Minimal Supersymmetric Standard Model featuring a non-minimal flavour violation in the second- and third-generation squark sector. The top squark in this model has two possible decay modes, either ${\stackrel{~}{t}}_{1}\to c{\stackrel{~}{\chi }}_{1}^{0}$ or ${\stackrel{~}{t}}_{1}\to t{\stackrel{~}{\chi }}_{1}^{0}$ , where the ${\stackrel{~}{\chi }}_{1}^{0}$ is undetected. The analysis is optimised assuming that both of the decay modes are equally probable, leading to the most likely final state of $\mathrm{tc}+{E}_{T}^{\text{miss}}$ . Good agreement is found between the Standard Model expectation and the data in the search regions. Exclusion limits at 95% CL are obtained in the $m\left({\stackrel{~}{t}}_{1}\right)$ vs. $m\left({\stackrel{~}{\chi }}_{1}^{0}\right)$ plane and, in addition, limits on the branching ratio of the ${\stackrel{~}{t}}_{1}\to t{\stackrel{~}{\chi }}_{1}^{0}$ decay as a function of m( ${\stackrel{~}{t}}_{1}$ ) are also produced. Top-squark masses of up to 800 GeV are excluded for scenarios with light neutralinos, and top-squark masses up to 600 GeV are excluded in scenarios where the neutralino and the top squark are almost mass degenerate.