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Determination of the strong coupling constant αs(mZ) in next-to-next-to-leading order QCD using H1 jet cross section measurements: H1 Collaboration

  • V. Andreev
  • , A. Baghdasaryan
  • , K. Begzsuren
  • , A. Belousov
  • , V. Bertone
  • , A. Bolz
  • , V. Boudry
  • , G. Brandt
  • , V. Brisson
  • , D. Britzger
  • , A. Buniatyan
  • , A. Bylinkin
  • , L. Bystritskaya
  • , A. J. Campbell
  • , K. B. Cantun Avila
  • , K. Cerny
  • , V. Chekelian
  • , J. G. Contreras
  • , J. Cvach
  • , J. Currie
  • J. B. Dainton, K. Daum, C. Diaconu, M. Dobre, V. Dodonov, G. Eckerlin, S. Egli, E. Elsen, L. Favart, A. Fedotov, J. Feltesse, M. Fleischer, A. Fomenko, E. Gabathuler, J. Gayler, T. Gehrmann, S. Ghazaryan, L. Goerlich, N. Gogitidze, M. Gouzevitch, C. Grab, A. Grebenyuk, T. Greenshaw, G. Grindhammer, C. Gwenlan, D. Haidt, R. C.W. Henderson, J. Hladkỳ, D. Hoffmann, R. Horisberger, T. Hreus, F. Huber, A. Huss, M. Jacquet, X. Janssen, A. W. Jung, H. Jung, M. Kapichine, J. Katzy, C. Kiesling, M. Klein, C. Kleinwort, R. Kogler, P. Kostka, J. Kretzschmar, D. Krücker, K. Krüger, M. P.J. Landon, W. Lange, P. Laycock, A. Lebedev, S. Levonian, K. Lipka, B. List, J. List, B. Lobodzinski, E. Malinovski, H. U. Martyn, S. J. Maxfield, A. Mehta, A. B. Meyer, H. Meyer, J. Meyer, S. Mikocki, A. Morozov, K. Müller, Th Naumann, P. R. Newman, C. Niebuhr, J. Niehues, G. Nowak, J. E. Olsson, D. Ozerov, C. Pascaud, G. D. Patel, E. Perez, A. Petrukhin, I. Picuric, H. Pirumov, D. Pitzl, R. Plačakytė, R. Polifka, K. Rabbertz, V. Radescu, N. Raicevic, T. Ravdandorj, P. Reimer, E. Rizvi, P. Robmann, R. Roosen, A. Rostovtsev, M. Rotaru, D. Šálek, D. P.C. Sankey, M. Sauter, E. Sauvan, S. Schmitt, L. Schoeffel, A. Schöning, F. Sefkow, S. Shushkevich, Y. Soloviev, P. Sopicki, D. South, V. Spaskov, A. Specka, M. Steder, B. Stella, U. Straumann, M. R. Sutton, T. Sykora, P. D. Thompson, D. Traynor, P. Truöl, I. Tsakov, B. Tseepeldorj, A. Valkárová, C. Vallée, P. Van Mechelen, Y. Vazdik, D. Wegener, E. Wünsch, J. ek, Z. Zhang, R. Žlebčík, H. Zohrabyan, F. Zomer
  • P.N. Lebedev Physical Institute of the Russian Academy of Sciences
  • Yerevan Physics Institute
  • Institute of Physics and Technology of the Mongolian Academy of Sciences
  • Vrije Universiteit Amsterdam
  • Science Park 105
  • University of Heidelberg
  • Georg-August-Universität Göttingen
  • Laboratoire de l'Accélérateur Linéaire
  • University of Birmingham
  • Moscow Institute of Physics and Technology
  • Institute for Theoretical and Experimental Physics
  • c/o DESY
  • Dept. Fis. Ap. CINVESTAV
  • Charles University
  • Max-Planck-Institut für Physik
  • Institute of Physics of the Czech Academy of Sciences
  • Durham University
  • University of Liverpool
  • Bergische Universität Gesamthochschule Wuppertal
  • Aix-Marseille Université
  • Horia Hulubei National Institute of Physics and Nuclear Engineering
  • Paul Scherrer Institut
  • Inter-University Institute for High Energies ULB-VUB
  • Universite Paris-Saclay
  • Physik-Institut der Universität Zürich
  • Institute for Nuclear Physics
  • IGFL, Université de Lyon, Université Lyon 1
  • ETH Zurich
  • University of Oxford
  • Lancaster University
  • Purdue University
  • Joint Institute for Nuclear Research, Dubna
  • Universität Hamburg
  • Queen Mary University of London
  • RWTH Aachen University
  • European Organization for Nuclear Research
  • University of Montenegro
  • University of Toronto
  • Institute of Meteorology and Climate Research
  • Institute for Information Transmission Problems (RAS)
  • CCLRC Rutherford Appleton Laboratory
  • Université Savoie Mont Blanc
  • Moscow State University
  • University Roma Tre
  • University of Sussex
  • Institute for Nuclear Research and Nuclear Energy Bulgarian Academy of Sciences
  • Ulaanbaatar University
  • University of Dortmund

Résultats de recherche: Contribution à un journalArticleRevue par des pairs

Résumé

The strong coupling constant αs is determined from inclusive jet and dijet cross sections in neutral-current deep-inelastic ep scattering (DIS) measured at HERA by the H1 collaboration using next-to-next-to-leading order (NNLO) QCD predictions. The dependence of the NNLO predictions and of the resulting value of αs(mZ) at the Z-boson mass mZ are studied as a function of the choice of the renormalisation and factorisation scales. Using inclusive jet and dijet data together, the strong coupling constant is determined to be αs(mZ)=0.1157(20)exp(29)th. Complementary, αs(mZ) is determined together with parton distribution functions of the proton (PDFs) from jet and inclusive DIS data measured by the H1 experiment. The value αs(mZ)=0.1142(28)tot obtained is consistent with the determination from jet data alone. The impact of the jet data on the PDFs is studied. The running of the strong coupling is tested at different values of the renormalisation scale and the results are found to be in agreement with expectations.

langue originaleAnglais
Numéro d'article791
journalEuropean Physical Journal C
Volume77
Numéro de publication11
Les DOIs
étatPublié - 1 nov. 2017

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