Skip to main navigation Skip to search Skip to main content

Diffractive dijet production with a leading proton in ep collisions at HERA

  • H1 collaboration The H1 collaboration
  • , V. Andreev
  • , A. Baghdasaryan
  • , K. Begzsuren
  • , A. Belousov
  • , P. Belov
  • , V. Boudry
  • , G. Brandt
  • , M. Brinkmann
  • , V. Brisson
  • , D. Britzger
  • , A. Buniatyan
  • , A. Bylinkin
  • , L. Bystritskaya
  • , A. J. Campbell
  • , K. B. Cantun Avila
  • , F. Ceccopieri
  • , K. Cerny
  • , V. Chekelian
  • , J. G. Contreras
  • J. Cvach, J. B. Dainton, K. Daum, C. Diaconu, M. Dobre, V. Dodonov, A. Dossanov, G. Eckerlin, S. Egli, E. Elsen, L. Favart, A. Fedotov, J. Feltesse, J. Ferencei, M. Fleischer, A. Fomenko, E. Gabathuler, J. Gayler, S. Ghazaryan, A. Glazov, L. Goerlich, N. Gogitidze, M. Gouzevitch, C. Grab, A. Grebenyuk, T. Greenshaw, G. Grindhammer, D. Haidt, R. C.W. Henderson, M. Herbst, J. Hladky, D. Hoffmann, R. Horisberger, T. Hreus, F. Huber, M. Jacquet, X. Janssen, H. Jung, M. Kapichine, C. Kiesling, M. Klein, C. Kleinwort, R. Kogler, P. Kostka, J. Kretzschmar, 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, G. Nowak, J. E. Olsson, D. Ozerov, P. Pahl, C. Pascaud, G. D. Patel, E. Perez, A. Petrukhin, I. Picuric, H. Pirumov, D. Pitzl, R. Plačakytė, B. Pokorny, R. Polifka, V. Radescu, N. Raicevic, T. Ravdandorj, P. Reimer, E. Rizvi, P. Robmann, R. Roosen, A. Rostovtsev, M. Rotaru, S. Rusakov, D. Šálek, D. P.C. Sankey, M. Sauter, E. Sauvan, S. Schmitt, L. Schoeffel, A. Schöning, H. C. Schultz-Coulon, F. Sefkow, S. Shushkevich, Y. Soloviev, P. Sopicki, D. South, V. Spaskov, A. Specka, M. Steder, B. Stella, U. Straumann, T. Sykora, P. D. Thompson, D. Traynor, P. Truöl, I. Tsakov, B. Tseepeldorj, J. Turnau, A. Valkárová, C. Vallée, P. Van Mechelen, Y. Vazdik, D. Wegener, E. Wünsch, J. Žáček, 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
  • c/o DESY
  • University of Oxford
  • Laboratoire de l'Accélérateur Linéaire
  • University of Birmingham
  • Institute for Theoretical and Experimental Physics
  • Moscow Institute of Physics and Technology
  • Dept. Fis. Ap. CINVESTAV
  • Inter-University Institute for High Energies ULB-VUB
  • Charles University
  • Max-Planck-Institut für Physik
  • Institute of Physics of the Czech Academy of Sciences
  • University of Liverpool
  • Bergische Universität Gesamthochschule Wuppertal
  • Aix Marseille Université
  • Horia Hulubei National Institute of Physics and Nuclear Engineering
  • Universität Hamburg
  • Paul Scherrer Institut
  • CEA/UVSQ/CNRS
  • Slovak Academy of Sciences
  • Institute for Nuclear Physics
  • IGFL, Université de Lyon, Université Lyon 1
  • ETH Zurich
  • Lancaster University
  • University of Heidelberg
  • Joint Institute for Nuclear Research, Dubna
  • Queen Mary University of London
  • RWTH Aachen University
  • Physik-Institut der Universität Zürich
  • European Organization for Nuclear Research
  • University of Montenegro
  • University of Toronto
  • CCLRC Rutherford Appleton Laboratory
  • Université Savoie Mont Blanc
  • University Roma Tre
  • Institute for Nuclear Research and Nuclear Energy Bulgarian Academy of Sciences
  • Ulaanbaatar University
  • University of Dortmund

Research output: Contribution to journalArticlepeer-review

23 Citations (Scopus)

Abstract

Abstract: The cross section of the diffractive process e+p → e+Xp is measured at a centre-of-mass energy of 318 GeV, where the system X contains at least two jets and the leading final state proton p is detected in the H1 Very Forward Proton Spectrometer. The measurement is performed in photoproduction with photon virtualities Q2< 2 GeV2 and in deep-inelastic scattering with 4 GeV2< Q2< 80 GeV2. The results are compared to next- to-leading order QCD calculations based on diffractive parton distribution functions as extracted from measurements of inclusive cross sections in diffractive deep-inelastic scattering.

Original languageEnglish
Article number56
JournalJournal of High Energy Physics
Volume2015
Issue number5
DOIs
Publication statusPublished - 16 May 2015

Keywords

  • Diffraction
  • Jets
  • Lepton-Nucleon Scattering
  • QCD

Fingerprint

Dive into the research topics of 'Diffractive dijet production with a leading proton in ep collisions at HERA'. Together they form a unique fingerprint.

Cite this