Measurement of the toverline{t} production cross-section in pp collisions at sqrt{s} = 5.02 TeV with the ATLAS detector

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Dallapiccola ,F He ,L Flores ,V Araujo Ferraz ,M Klassen ,Š Todorova-Nová ,O Jinnouchi ,J Stark ,Evan Michael Carlson ,H J Lubatti ,M Citterio ,P Zhao ,J Jamieson ,D Reikher ,V O Tikhomirov ,O E Vickey Boeriu ,Y Nakahama ,C Wiel ,C Moreno Martínez ,B Moser ,R J Hawkings ,A Petukhov ,C Sbarra ,P Tipton ,T Wang ,J Walder ,K Karava ,Sreelakshmi Sindhu ,S Möbius ,A Di Girolamo ,A Olszewski ,Barbora Eckerova ,D Zanzi ,A M Burger ,W J Fawcett ,D Robinson ,A Lucotte ,K Assamagan ,H Krüger ,T Vazquez Schroeder ,L Diehl ,X Chen ,Kamal Saoucha ,F Del Corso ,M Lassnig ,G L Alberghi ,Kyle Stuart Krowpman ,Z Marshall ,J Roggel ,D Salvatore ,D Boumediene ,G Unal ,T J Min ,Bryn Arthur Roberts ,A M Lory ,L Massa ,P Massarotti ,G Padovano ,P D Thompson ,Z Zheng ,J L Oliver ,G Cowan ,P Kramer ,E W Parrish ,T Iizawa ,B S Acharya ,M Liu ,X Wang ,D M S Sultan ,J Heilman ,M Kuze ,M Guth ,J E García Navarro ,L Chevalier ,N Viaux Maira ,Jonas Steentoft ,Easwar Anand Narayanan ,M Ellert ,Haruka Asada ,Greg 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P Denisov ,M Antonelli ,D P Mungo ,H M Gray ,A Ivina ,I Hinchliffe ,R Gamboa Goni ,A Roy ,J K Behr ,D M Mac Donell ,B Achkar ,B P Nachman ,Mpho Gift Doctor Gololo ,H Li ,E P Takeva ,D Sperlich ,C A Gottardo ,S Morgenstern ,C Weiser ,L Masetti ,Huan Pang ,E J W Moyse ,Maheyer Jamshed Shroff ,E Celebi ,S Amoroso ,Ksenia Solovieva ,G Brooijmans ,E Antipov ,G Navarro ,H Ito ,Marco Cristoforetti ,X Wang ,Bastian Schlag ,S González-Sevilla ,M Mikeštíková ,M Geisen ,Jack Joseph Hall ,S Oerdek ,M Tsopoulou ,R A Mcpherson ,J Guo ,R Bielski ,S Giagu ,I A Minashvili ,I Vivarelli ,C Wang ,P M Tuts ,R Hertenberger ,A Soffer ,F Conventi ,L Castillo García ,Ota Zaplatilek ,Maciej Piotr Lewicki ,M Dunford ,H P Beck ,J Shojaii ,C Leggett ,S Menke ,L Brenner ,R M Jacobs ,Micael Verissimo De Araujo ,N Yamaguchi ,M W Krasny ,F Djama ,P Martinez Agullo ,A Carbone ,G A Vasquez ,D Scheirich ,R De Asmundis ,J Sjölin ,D Sengupta ,J Novák ,M Dyndał ,S M Gibson ,W Wiedenmann ,P Bussey ,A Dimitrievska ,S Todt ,N 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doi:10.1007/jhep06(2023)138

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https://doi.org/10.1007/jhep06(2023)138

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Journal: Journal of High Energy Physics	Publication Date: Jun 23, 2023
Citations: 1	License type: CC BY 4.0

Abstract

The inclusive top-quark pair ( toverline{t} ) production cross-section {sigma}_{toverline{t}} is measured in proton–proton collisions at a centre-of-mass energy sqrt{s} = 5.02 TeV, using 257 pb−1 of data collected in 2017 by the ATLAS experiment at the LHC. The toverline{t} cross-section is measured in both the dilepton and single-lepton final states of the toverline{t} system and then combined. The combination of the two measurements yieldsσtt¯=67.5±0.9stat.±2.3syst.±1.1lumi.±0.2beampb,\\documentclass[12pt]{minimal} \\usepackage{amsmath} \\usepackage{wasysym} \\usepackage{amsfonts} \\usepackage{amssymb} \\usepackage{amsbsy} \\usepackage{mathrsfs} \\usepackage{upgreek} \\setlength{\\oddsidemargin}{-69pt} \\begin{document}$$ {\\sigma}_{t\\overline{t}}=67.5\\pm 0.9\\left(\ extrm{stat}.\\right)\\pm 2.3\\left(\ extrm{syst}.\\right)\\pm 1.1\\left(\ extrm{lumi}.\\right)\\pm 0.2\\left(\ extrm{beam}\\right)\ extrm{pb}, $$\\end{document}where the four uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, and imperfect knowledge of both the integrated luminosity and the LHC beam energy, giving a total uncertainty of 3.9%. The result is in agreement with theoretical quantum chromodynamic calculations at next-to-next-to-leading order in the strong coupling constant, including the resummation of next-to-next-to-leading logarithmic soft-gluon terms, and constrains the parton distribution functions of the proton at large Bjorken-x.

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