Abstract
The inclusive top quark pair (tt¯) production cross-section σtt¯ has been measured in proton–proton collisions at √s = 13TeV, using 36.1 fb-1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge eμ pair and b-tagged jets, the cross-section is measured to be: σtt¯= 826.4 ± 3.6(stat) ± 11.5(syst) ± 15.7(lumi) ± 1.9(beam)pb, where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on mtpole, giving mtpole = 173.1-2.1+2.0 GeV. It is also combined with measurements at √s = 7 TeV and √s = 8 TeV to derive ratios and double ratios of tt¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.
Original language | English |
---|---|
Article number | 528 |
Pages (from-to) | 1-70 |
Number of pages | 70 |
Journal | European Physical Journal C |
Volume | 80 |
Issue number | 6 |
DOIs | |
Publication status | Published - Jun 2020 |
Externally published | Yes |
Bibliographical note
Copyright the Author(s) 2020. Version archived for private and non-commercial use with the permission of the author/s and according to publisher conditions. For further rights please contact the publisher.Cite this
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In: European Physical Journal C, Vol. 80, No. 6, 528, 06.2020, p. 1-70.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Measurement of the tt¯ production cross-section and lepton differential distributions in eμ dilepton events from pp collisions at √s = 13TeV with the ATLAS detector
AU - ATLAS Collaboration
AU - Aad, G.
AU - Abbott, B.
AU - Abbott, D. C.
AU - Abud, A. Abed
AU - Abeling, K.
AU - Abhayasinghe, D. K.
AU - Abidi, S. H.
AU - AbouZeid, O. S.
AU - Abraham, N. L.
AU - Abramowicz, H.
AU - Abreu, H.
AU - Abulaiti, Y.
AU - Acharya, B. S.
AU - Achkar, B.
AU - Adachi, S.
AU - Adam, L.
AU - Bourdarios, C. Adam
AU - Adamczyk, L.
AU - Adamek, L.
AU - Adelman, J.
AU - Adersberger, M.
AU - Adiguzel, A.
AU - Adorni, S.
AU - Adye, T.
AU - Affolder, A. A.
AU - Afik, Y.
AU - Agapopoulou, C.
AU - Agaras, M. N.
AU - Aggarwal, A.
AU - Agheorghiesei, C.
AU - Aguilar-Saavedra, J. A.
AU - Ahmadov, F.
AU - Ahmed, W. S.
AU - Ai, X.
AU - Aielli, G.
AU - Akatsuka, S.
AU - Åkesson, T. P.A.
AU - Akilli, E.
AU - Akimov, A. V.
AU - Khoury, K. Al
AU - Alberghi, G. L.
AU - Albert, J.
AU - Verzini, M. J.Alconada
AU - Alderweireldt, S.
AU - Aleksa, M.
AU - Aleksandrov, I. N.
AU - Alexa, C.
AU - Alexopoulos, T.
AU - Alfonsi, A.
AU - Alfonsi, F.
AU - Alhroob, M.
AU - Ali, B.
AU - Aliev, M.
AU - Alimonti, G.
AU - Alkire, S. P.
AU - Allaire, C.
AU - Allbrooke, B. M.M.
AU - Allen, B. W.
AU - Allport, P. P.
AU - Aloisio, A.
AU - Alonso, A.
AU - Alonso, F.
AU - Alpigiani, C.
AU - Alshehri, A. A.
AU - Estevez, M. Alvarez
AU - Piqueras, D. Álvarez
AU - Alviggi, M. G.
AU - Coutinho, Y. Amaral
AU - Ambler, A.
AU - Ambroz, L.
AU - Amelung, C.
AU - Amidei, D.
AU - Santos, S. P.Amor Dos
AU - Amoroso, S.
AU - Amrouche, C. S.
AU - An, F.
AU - Anastopoulos, C.
AU - Andari, N.
AU - Andeen, T.
AU - Anders, C. F.
AU - Anders, J. K.
AU - Andreazza, A.
AU - Andrei, V.
AU - Anelli, C. R.
AU - Angelidakis, S.
AU - Angerami, A.
AU - Anisenkov, A. V.
AU - Annovi, A.
AU - Antel, C.
AU - Anthony, M. T.
AU - Antipov, E.
AU - Antonelli, M.
AU - Antrim, D. J.A.
AU - Anulli, F.
AU - Aoki, M.
AU - Pozo, J. A.Aparisi
AU - Bella, L. Aperio
AU - Araque, J. P.
AU - Ferraz, V. Araujo
AU - Pereira, R. Araujo
AU - Arcangeletti, C.
AU - Arce, A. T.H.
AU - Arduh, F. A.
AU - Arguin, J. F.
AU - Argyropoulos, S.
AU - Arling, J. H.
AU - Armbruster, A. J.
AU - Armstrong, A.
AU - Arnaez, O.
AU - Arnold, H.
AU - Tame, Z. P.Arrubarrena
AU - Artoni, G.
AU - Artz, S.
AU - Asai, S.
AU - Asbah, N.
AU - Asimakopoulou, E. M.
AU - Asquith, L.
AU - Assahsah, J.
AU - Assamagan, K.
AU - Astalos, R.
AU - Atkin, R. J.
AU - Atkinson, M.
AU - Atlay, N. B.
AU - Atmani, H.
AU - Augsten, K.
AU - Avolio, G.
AU - Avramidou, R.
AU - Ayoub, M. K.
AU - Azoulay, A. M.
AU - Azuelos, G.
AU - Bachacou, H.
AU - Bachas, K.
AU - Backes, M.
AU - Backman, F.
AU - Bagnaia, P.
AU - Bahmani, M.
AU - Bahrasemani, H.
AU - Bailey, A. J.
AU - Bailey, V. R.
AU - Baines, J. T.
AU - Bajic, M.
AU - Bakalis, C.
AU - Baker, O. K.
AU - Bakker, P. J.
AU - Gupta, D. Bakshi
AU - Balaji, S.
AU - Baldin, E. M.
AU - Balek, P.
AU - Balli, F.
AU - Balunas, W. K.
AU - Balz, J.
AU - Banas, E.
AU - Bandyopadhyay, A.
AU - Banerjee, Sw
AU - Bannoura, A. A.E.
AU - Barak, L.
AU - Barbe, W. M.
AU - Barberio, E. L.
AU - Barberis, D.
AU - Barbero, M.
AU - Barbour, G.
AU - Barillari, T.
AU - Barisits, M. S.
AU - Barkeloo, J.
AU - Barklow, T.
AU - Barnea, R.
AU - Barnes, S. L.
AU - Barnett, B. M.
AU - Barnett, R. M.
AU - Barnovska-Blenessy, Z.
AU - Baroncelli, A.
AU - Barone, G.
AU - Barr, A. J.
AU - Navarro, L. Barranco
AU - Barreiro, F.
AU - da Costa, J. Barreiro Guimarães
AU - Barsov, S.
AU - Bartoldus, R.
AU - Bartolini, G.
AU - Barton, A. E.
AU - Bartos, P.
AU - Basalaev, A.
AU - Basan, A.
AU - Bassalat, A.
AU - Basso, M. J.
AU - Bates, R. L.
AU - Batlamous, S.
AU - Batley, J. R.
AU - Batool, B.
AU - Battaglia, M.
AU - Bauce, M.
AU - Bauer, F.
AU - Bauer, K. T.
AU - Bawa, H. S.
AU - Beacham, J. B.
AU - Beau, T.
AU - Beauchemin, P. H.
AU - Becherer, F.
AU - Bechtle, P.
AU - Beck, H. C.
AU - Beck, H. P.
AU - Becker, K.
AU - Becker, M.
AU - Becot, C.
AU - Beddall, A. J.
AU - Beddall, A. J.
AU - Bednyakov, V. A.
AU - Bedognetti, M.
AU - Bee, C. P.
AU - Beermann, T. A.
AU - Begalli, M.
AU - Begel, M.
AU - Behera, A.
AU - Behr, J. K.
AU - Beisiegel, F.
AU - Bell, A. S.
AU - Bella, G.
AU - Bellagamba, L.
AU - Bellerive, A.
AU - Bellos, P.
AU - Beloborodov, K.
AU - Belotskiy, K.
AU - Belyaev, N. L.
AU - Benchekroun, D.
AU - Benekos, N.
AU - Benhammou, Y.
AU - Benjamin, D. P.
AU - Benoit, M.
AU - Bensinger, J. R.
AU - Bentvelsen, S.
AU - Beresford, L.
AU - Beretta, M.
AU - Berge, D.
AU - Kuutmann, E. Bergeaas
AU - Berger, N.
AU - Bergmann, B.
AU - Bergsten, L. J.
AU - Beringer, J.
AU - Berlendis, S.
AU - Bernardi, G.
AU - Bernius, C.
AU - Bernlochner, F. U.
AU - Berry, T.
AU - Berta, P.
AU - Bertella, C.
AU - Bertram, I. A.
AU - Bylund, O. Bessidskaia
AU - Besson, N.
AU - Bethani, A.
AU - Shojaii, J.
N1 - Copyright the Author(s) 2020. Version archived for private and non-commercial use with the permission of the author/s and according to publisher conditions. For further rights please contact the publisher.
PY - 2020/6
Y1 - 2020/6
N2 - The inclusive top quark pair (tt¯) production cross-section σtt¯ has been measured in proton–proton collisions at √s = 13TeV, using 36.1 fb-1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge eμ pair and b-tagged jets, the cross-section is measured to be: σtt¯= 826.4 ± 3.6(stat) ± 11.5(syst) ± 15.7(lumi) ± 1.9(beam)pb, where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on mtpole, giving mtpole = 173.1-2.1+2.0 GeV. It is also combined with measurements at √s = 7 TeV and √s = 8 TeV to derive ratios and double ratios of tt¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.
AB - The inclusive top quark pair (tt¯) production cross-section σtt¯ has been measured in proton–proton collisions at √s = 13TeV, using 36.1 fb-1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge eμ pair and b-tagged jets, the cross-section is measured to be: σtt¯= 826.4 ± 3.6(stat) ± 11.5(syst) ± 15.7(lumi) ± 1.9(beam)pb, where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on mtpole, giving mtpole = 173.1-2.1+2.0 GeV. It is also combined with measurements at √s = 7 TeV and √s = 8 TeV to derive ratios and double ratios of tt¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.
UR - http://www.scopus.com/inward/record.url?scp=85086475740&partnerID=8YFLogxK
U2 - 10.1140/epjc/s10052-020-7907-9
DO - 10.1140/epjc/s10052-020-7907-9
M3 - Article
AN - SCOPUS:85086475740
SN - 1434-6052
VL - 80
SP - 1
EP - 70
JO - European Physical Journal C
JF - European Physical Journal C
IS - 6
M1 - 528
ER -