2020
DOI: 10.1140/epjc/s10052-020-08509-3
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Evidence for $$t\bar{t}t\bar{t}$$ production in the multilepton final state in proton–proton collisions at $$\sqrt{s}=13$$ $$\text {TeV}$$ with the ATLAS detector

Abstract: A search is presented for four-top-quark production using an integrated luminosity of 139 fb$$^{-1}$$ - 1 of proton–proton collision data at a centre-of-mass energy of $$13~\text {TeV}$$ 13 TeV collected by the ATLAS detector at the LHC. Events are selected if they contain a same-sign lepton pair or at least three leptons (electrons or muons). Jet multiplicity, jet flavour and event kinematics are used to separate signal from the background through a multivariate discriminant, and dedicated control r… Show more

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Cited by 62 publications
(89 citation statements)
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“…A similar bound is obtained by CMS [18]. Besides, very recently both experiments have updated their multilepton searches to ≈ 140 fb −1 [22,23], observing mild but intriguing excesses with respect to the SM predictions; we will discuss these separately in section 3. Constraints comparable to the one on c tt are obtained for the full set of four-top operators [18], which also involve the third generation left-handed quark doublet,…”
Section: Operators Expectations and Current Constraintssupporting
confidence: 68%
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“…A similar bound is obtained by CMS [18]. Besides, very recently both experiments have updated their multilepton searches to ≈ 140 fb −1 [22,23], observing mild but intriguing excesses with respect to the SM predictions; we will discuss these separately in section 3. Constraints comparable to the one on c tt are obtained for the full set of four-top operators [18], which also involve the third generation left-handed quark doublet,…”
Section: Operators Expectations and Current Constraintssupporting
confidence: 68%
“…2. The ATLAS four-top measurement [23] finds σ tttt = 24 +7 −6 fb, and also observes an excess of ttW events relative to the SM reference, with best fit µ ttW = 1.6 ± 0.3 based on σ SM, R ttW = 601 fb. The normalization of ttZ is not left to vary in the fit.…”
Section: Jhep02(2021)043mentioning
confidence: 89%
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“…Previous similar studies have concentrated on narrower (r < 0.2) resonances [17,18], or tried to fit the large forward-backward (FB) asymmetry at the Tevatron using decay channels involving top-quark partners [19][20][21], or considered the case of KK resonances in the electroweak (model dependent) sector, which then allows lepton channels as possible final states [22,23]. We will also apply our theoretical results to the study of other final state channels, in particular to ttW , ttZ, ttH, and tttt, whose experimental detection is currently work in progress [24][25][26][27][28][29].…”
Section: Introductionmentioning
confidence: 99%