A measurement of the associated production of a top-quark pair (𝑡 ¯ 𝑡 ) with a vector boson (𝑊, 𝑍) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The 𝑡 ¯ 𝑡 𝑍 and 𝑡 ¯ 𝑡 𝑊 production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are 𝜎𝑡 ¯ 𝑡 𝑍=0.95±0.08stat±0.10syst pb and 𝜎𝑡 ¯ 𝑡 𝑊=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the 𝑡 ¯ 𝑡 𝑍 cross section is used to set constraints on effective field theory operators which modify the 𝑡 ¯ 𝑡 𝑍 vertex.
Aaboud M., A.G. (2019). Measurement of the 𝑡¯𝑡𝑍 and 𝑡¯𝑡𝑊 cross sections in proton-proton collisions at √𝑠=13 TeV with the ATLAS detector. PHYSICAL REVIEW D, 99(7), 072009-1-072009-38 [10.1103/PhysRevD.99.072009].
Measurement of the 𝑡¯𝑡𝑍 and 𝑡¯𝑡𝑊 cross sections in proton-proton collisions at √𝑠=13 TeV with the ATLAS detector
Alberghi G. L.;Bellagamba L.;Bindi M.;Boscherini D.;Cabras G.;Caforio D.;De Castro S.;Derkaoui J. E.;Di Donato C.;Di Nardo R.;Di Sipio R.;Evans H.;Fabbri F.;Fabbri L.;Franchini M.;Gabrielli A.;Giacobbe B.;Lasagni Manghi F.;Macchiolo A.;Massa L.;Monzani S.;Polini A.;Rinaldi L.;Romano M.;Sbarra C.;Sbrizzi A.;Semprini-Cesari N.;Sioli M.;Todome K.;Ucchielli G.;Valentinetti S.;Villa M.;Vittori C.;Vivarelli I.;Zoccoli A.;
2019
Abstract
A measurement of the associated production of a top-quark pair (𝑡 ¯ 𝑡 ) with a vector boson (𝑊, 𝑍) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The 𝑡 ¯ 𝑡 𝑍 and 𝑡 ¯ 𝑡 𝑊 production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are 𝜎𝑡 ¯ 𝑡 𝑍=0.95±0.08stat±0.10syst pb and 𝜎𝑡 ¯ 𝑡 𝑊=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the 𝑡 ¯ 𝑡 𝑍 cross section is used to set constraints on effective field theory operators which modify the 𝑡 ¯ 𝑡 𝑍 vertex.File | Dimensione | Formato | |
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