Ústav technické a experimentální fyziky Institute of Experimental and Applied Physics

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

NázevTitle
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 detectorA 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
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
G. Aad, B. Abbott, K. Abeling, N. J. Abicht, B. Ali, K. Augsten, B. Bergmann, H. Day-Hall, P. Fiedler, Z. Hubáček, P. Jačka, S. Mondal, M. Myška, L. Novotný, V. Petousis, R. Polifka, S. Pospíšil, K. Smolek, A. Sopczak, V. Vacek, P. Vokáč, O. Zaplatílek
DOIDOI
10.1007/JHEP07(2024)250
Časopis / citaceJournal / citation
Journal of High Energy Physics. 2024, 2024(7), ISSN 1029-8479.
RokYear
2024
JazykLanguage
eng
WoSWoS
001426790900001
ScopusScopus
2-s2.0-85200565461
RIVRIV
RIV/68407700:21220/24:00390182!RIV26-MSM-21220___
ProjektProject
CERN-CZ III - Výzkumná infrastruktura pro experimenty v CERN - LM2023040 (2023–2026)CERN-CZ III - Výzkumná infrastruktura pro experimenty v CERN - LM2023040 (2023–2026); Institucionální podpora na rozvoj výzkumné org.Institucionální podpora na rozvoj výzkumné org.; Výzkum základních stavebních kamenů hmoty s využitím špičkových technologiíFundamental constituents of matter through frontier technologies

AbstraktAbstract

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 root s = 13TeV. 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 (t) over tilde (1) -> c (chi) over tilde (0)(1) or (t) over tilde (1) -> t (chi) over tilde (0)(1), where the (chi) over tilde (0)(1) is undetected. The analysis is optimised assuming that both of the decay modes are equally probable, leading to the most likely final state of tc + E-T(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((t) over tilde1) vs . m((chi) over tilde (0)(1)) plane and, in addition, limits on the branching ratio of the (t) over tilde -> t (chi) over tilde (0)(1)1 decay as a function of m((t) over tilde (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.

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 root s = 13TeV. 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 (t) over tilde (1) -> c (chi) over tilde (0)(1) or (t) over tilde (1) -> t (chi) over tilde (0)(1), where the (chi) over tilde (0)(1) is undetected. The analysis is optimised assuming that both of the decay modes are equally probable, leading to the most likely final state of tc + E-T(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((t) over tilde1) vs . m((chi) over tilde (0)(1)) plane and, in addition, limits on the branching ratio of the (t) over tilde -> t (chi) over tilde (0)(1)1 decay as a function of m((t) over tilde (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.