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Exclusive ρ0 meson photoproduction with a leading neutron at HERA: H1 Collaboration

  • V. Andreev
  • , A. Baghdasaryan
  • , K. Begzsuren
  • , A. Belousov
  • , 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. B. Dainton
  • , K. Daum
  • C. Diaconu, M. Dobre, V. Dodonov, G. Eckerlin, S. Egli, E. Elsen, L. Favart, A. Fedotov, J. Feltesse, J. Ferencei, M. Fleischer, A. Fomenko, E. Gabathuler, J. Gayler, S. Ghazaryan, L. Goerlich, N. Gogitidze, M. Gouzevitch, C. Grab, A. Grebenyuk, T. Greenshaw, G. Grindhammer, D. Haidt, R. C.W. Henderson, J. Hladkỳ, 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, C. Pascaud, G. D. Patel, E. Perez, A. Petrukhin, I. Picuric, H. Pirumov, D. Pitzl, R. Plačakytė, B. Pokorny, R. Polifka, B. Povh, 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, 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
  • University of Heidelberg
  • Université Paris-Sud
  • Georg-August-Universität Göttingen
  • Laboratoire de l'Accélérateur Linéaire
  • c/o DESY
  • University of Birmingham
  • Institute for Theoretical and Experimental Physics
  • Moscow Institute of Physics and Technology
  • CINVESTAV-IPN
  • 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
  • Paul Scherrer Institut
  • Inter-University Institute for High Energies ULB-VUB
  • Universite Paris-Saclay
  • Institute of Experimental Physics Slovak Academy of Sciences
  • Institute for Nuclear Physics
  • IGFL, Université de Lyon, Université Lyon 1
  • ETH Zurich
  • Lancaster University
  • Joint Institute for Nuclear Research, Dubna
  • Universität Hamburg
  • Queen Mary University of London
  • RWTH Aachen University
  • Physik-Institut der Universität Zürich
  • European Organization for Nuclear Research
  • University of Montenegro
  • University of Toronto
  • Max-Planck-Institut für Kernphysik
  • Institute for Information Transmission Problems (RAS)
  • 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

Résultats de recherche: Contribution à un journalArticleRevue par des pairs

22 Citations (Scopus)

Résumé

A first measurement is presented of exclusive photoproduction of ρ0 mesons associated with leading neutrons at HERA. The data were taken with the H1 detector in the years 2006 and 2007 at a centre-of-mass energy of √s=319 GeV and correspond to an integrated luminosity of 1.16 pb-1. The ρ0 mesons with transverse momenta (Formula presented.) GeV are reconstructed from their decays to charged pions, while leading neutrons carrying a large fraction of the incoming proton momentum, (Formula presented.), are detected in the Forward Neutron Calorimeter. The phase space of the measurement is defined by the photon virtuality (Formula presented.), the total energy of the photon–proton system (Formula presented.) GeV and the polar angle of the leading neutron (Formula presented.)0.75 mrad. The cross section of the reaction (Formula presented.) is measured as a function of several variables. The data are interpreted in terms of a double peripheral process, involving pion exchange at the proton vertex followed by elastic photoproduction of a ρ0 meson on the virtual pion. In the framework of one-pion-exchange dominance the elastic cross section of photon-pion scattering, (Formula presented.), is extracted. The value of this cross section indicates significant absorptive corrections for the exclusive reaction (Formula presented.).

langue originaleAnglais
Numéro d'article41
Pages (de - à)1-21
Nombre de pages21
journalEuropean Physical Journal C
Volume76
Numéro de publication1
Les DOIs
étatPublié - 1 janv. 2016
Modification externeOui

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