Sensitivity of the Three Top Quark Production Process to the Contribution of Top-Related SMEFT Operators

The sensitivity of the three top quark production process to the potential contribution of the SMEFT top-related operators was investigated. Theoretical restrictions on the Wilson coefficients of the corresponding operators are obtained for the scenarios of the LHC, HL-LHC, HE-LHC, and FCC experiments. It is shown how these restrictions change with increasing energies and luminosities of the considered scenarios. It was demonstrated that the process constrains the following four-fermion operators relatively well: $$O_{{QQ}}^{1}$$ , $$O_{{Qq}}^{{1,8}}$$ , $$O_{{Qq}}^{{1,1}}$$ , $$O_{{Qq}}^{{3,8}}$$ , $$O_{{Qq}}^{{1,3}}$$ , $$O_{{Qt}}^{1}$$ , $$O_{{tq}}^{8}$$ , and it is also sensitive to the following operators with bosonic fields: $${{O}_{{tW}}}$$ and $${{O}_{{tG}}}$$ .

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Publication Details

Journal
Physics of Particles and Nuclei
Published
2025-04-01
DOI
https://doi.org/10.1134/s1063779624701661
Citations
1
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
1.87
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article

Sensitivity of the Three Top Quark Production Process to the Contribution of Top-Related SMEFT Operators

A. Aleshko, L. Dudko, V. Bunichev, E. E. Boos
1 citations
Physics of Particles and Nuclei
Particle physics theoretical and experimental studies
1.87
article

Sensitivity of the Three Top Quark Production Process to the Contribution of Top-Related SMEFT Operators

A. Aleshko, L. Dudko, V. Bunichev, E. E. Boos
article en
1 citations

Abstract

The sensitivity of the three top quark production process to the potential contribution of the SMEFT top-related operators was investigated. Theoretical restrictions on the Wilson coefficients of the corresponding operators are obtained for the scenarios of the LHC, HL-LHC, HE-LHC, and FCC experiments. It is shown how these restrictions change with increasing energies and luminosities of the considered scenarios. It was demonstrated that the process constrains the following four-fermion operators relatively well: $$O_{{QQ}}^{1}$$ , $$O_{{Qq}}^{{1,8}}$$ , $$O_{{Qq}}^{{1,1}}$$ , $$O_{{Qq}}^{{3,8}}$$ , $$O_{{Qq}}^{{1,3}}$$ , $$O_{{Qt}}^{1}$$ , $$O_{{tq}}^{8}$$ , and it is also sensitive to the following operators with bosonic fields: $${{O}_{{tW}}}$$ and $${{O}_{{tG}}}$$ .

Physics of Particles and NucleiVol. 56(2)
Lomonosov Moscow State University (RU)
Openalex Percentile: Top 14%
Particle physics theoretical and experimental studies
1.87
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