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Photoproduction with a leading proton at HERA

Authors :
Adloff, C
Andreev, V
Andrieu, B
Anthonis, T
Arkadov, V
Astvatsatourov, A
Ayyaz, I
Babaev, A
Bahr, J
Baranov, P
Barrelet, E
Bartel, W
Bate, P
Beglarian, A
Behnke, O
Beier, C
Belousov, A
Benisch, T
Berger, C
Berndt, T
Bizot, JC
Boudry, V
Braunschweig, W
Brisson, V
Broker, HB
Brown, DP
Bruckner, W
Bruel, P
Bruncko, D
Burger, J
Busser, FW
Bunyatyan, A
Burkhardt, H
Burrage, A
Buschhorn, G
Campbell, AJ
Cao, J
Carli, T
Caron, S
Chabert, E
Clarke, D
Clerbaux, B
Collard, C
Contreras, JG
Coppens, YR
Coughlan, JA
Cousinou, MC
Cox, BE
Cozzika, G
Cvach, J
Dainton, JB
Dau, WD
Daum, K
Davidsson, M
Delcourt, B
Delerue, N
Demirchyan, R
De Roeck, A
De Wolf, EA
Diaconu, C
Dixon, P
Dodonov, V
Dowell, JD
Droutskoi, A
Duprel, C
Eckerlin, G
Eckstein, D
Efremenko, V
Egli, S
Eichler, R
Eisele, F
Eisenhandler, E
Ellerbrock, M
Elsen, E
Erdmann, M
Erdmann, W
Faulkner, PJW
Favart, L
Fedotov, E
Felst, R
Ferencei, J
Ferron, S
Fleischer, M
Fleming, YH
Flugge, G
Fomenko, A
Foresti, I
Formanek, J
Foster, JM
Franke, G
Gabathuler, E
Gabathuler, K
Garvey, J
Gassner, J
Gayler, J
Gerhards, R
Ghazaryan, S
Goerlich, L
Gogitidze, N
Goldberg, M
Goodwin, C
Grab, C
Grassler, H
Greenshaw, T
Grindhammer, G
Hadig, T
Haidt, D
Hajduk, L
Haynes, WJ
Heinemann, B
Heinzelmann, G
Henderson, RCW
Hengstmann, S
Henschel, H
Heremans, R
Herrera, G
Herynek, I
Hildebrandt, M
Hilgers, M
Hiller, KH
Hladky, J
Hoting, P
Hoffmann, D
Horisberger, R
Hurling, S
Ibbotson, M
Issever, C
Jacquet, M
Jaffre, M
Janauschek, L
Jansen, DM
Janssen, X
Jemanov, V
Jonsson, L
Johnson, DP
Jones, MAS
Jung, H
Kastli, HK
Kant, D
Kapichine, M
Karlsson, M
Karschnick, O
Keil, F
Keller, N
Kennedy, J
Kenyon, IR
Kermiche, S
Kiesling, C
Kjellberg, P
Klein, M
Kleinwort, C
Knies, G
Koblitz, B
Kolya, SD
Korbel, V
Kostka, P
Kotelnikov, SK
Koutouev, R
Koutov, A
Krasny, MW
Krehbiel, H
Kroseberg, J
Kruger, K
Kupper, A
Kuhr, T
Kurca, T
Lahmann, R
Lamb, D
Landon, MPJ
Lange, W
Lastovicka, T
Laycock, P
Lebailly, E
Lebedev, A
Leissner, B
Lemrani, R
Lendermann, V
Levonian, S
Lindstroem, M
List, B
Lobodzinska, E
Lobodzinski, B
Loginov, A
Loktionova, N
Lubimov, V
Luders, S
Luke, D
Lytkin, L
Magnussen, N
Mahlke-Kruger, H
Malden, N
Malinovski, E
Malinovski, I
Maracek, R
Marage, P
Marks, J
Marshall, R
Martyn, HU
Martyniak, J
Maxfield, SJ
Mehta, A
Meier, K
Merkel, P
Meyer, AB
Meyer, H
Meyer, J
Meyer, PO
Mikocki, S
Milstead, D
Mkrtchyan, T
Mohr, R
Mohrdieck, S
Mondragon, MN
Moreau, F
Morozov, A
Morris, JV
Muller, K
Murin, P
Nagovizin, V
Naroska, B
Naumann, J
Naumann, T
Nellen, G
Newman, PR
Nicholls, TC
Niebergall, F
Niebuhr, C
Nix, O
Nowak, G
Nunnemann, T
Olsson, JE
Ozerov, D
Panassik, V
Pascaud, C
Patel, GD
Perez, E
Phillips, JP
Pitzl, D
Poschl, R
Potachnikova, I
Povh, B
Rabbertz, K
Radel, G
Rauschenberger, J
Reimer, P
Reisert, B
Reyna, D
Riess, S
Risler, C
Rizvi, E
Robmann, P
Roosen, R
Rostovtsev, A
Royon, C
Rusakov, S
Rybicki, K
Sankey, DPC
Scheins, J
Schilling, FP
Schleper, P
Schmidt, D
Schmitt, S
Schoeffel, L
Schoning, A
Schorner, T
Schroder, V
Schultz-Coulon, HC
Schwanenberger, C
Sedlak, K
Sefkow, F
Shekelyan, V
Sheviakov, I
Shtarkov, LN
Sievers, P
Sirois, Y
Sloan, T
Smirnov, P
Solochenko, V
Soloviev, Y
Spaskov, V
Specka, A
Spitzer, H
Stamen, R
Steinhart, J
Stella, B
Stellberger, A
Stiewe, J
Straumann, U
Struczinski, W
Swart, M
Tasevsky, M
Tchernyshov, V
Tchetchelnitski, S
Thompson, G
Thompson, PD
Tobien, N
Traynor, D
Truol, P
Tsipolitis, G
Tsurin, I
Turnau, J
Turney, JE
Tzamariudaki, E
Udluft, S
Usik, A
Valkar, S
Valkarova, A
Vallee, C
Van Mechelen, P
Vassiliev, S
Vazdik, Y
Vichnevski, A
Wacker, K
Wallny, R
Walter, T
Waugh, B
Weber, G
Weber, M
Wegener, D
Werner, M
White, G
Wiesand, S
Wilksen, T
Winde, M
Winter, GG
Wissing, C
Wobisch, M
Wollatz, H
Wunsch, E
Wyatt, AC
Zacek, J
Zalesak, J
Zhang, Z
Zhokin, A
Zomer, F
Zsembery, J
zur Nedden, M
Collaboration, H
Laboratoire Leprince-Ringuet (LLR)
Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE)
Centre National de la Recherche Scientifique (CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Pierre et Marie Curie - Paris 6 (UPMC)
Laboratoire de l'Accélérateur Linéaire (LAL)
Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)
Centre de Physique des Particules de Marseille (CPPM)
Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
H1
Kerec, Hélène
H1 Collaboration
Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS)
Université Pierre et Marie Curie - Paris 6 (UPMC)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)
Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
Source :
Nuclear Physics B, Nuclear Physics B, Elsevier, 2001, 619, pp.3-21, Nuclear physics : B, ResearcherID, Nuclear Physics B, 2001, 619, pp.3-21
Publication Year :
2001
Publisher :
HAL CCSD, 2001.

Abstract

The total cross section for the photoproduction process with a leading proton in the final state has been measured at gamma p centre-of-mass energies W of 91, 181 and 231 GeV. The measured cross sections apply to the kinematic range with the transverse momentum of the scattered proton restricted to p_Tproton Xp')(W,z)/dz is observed to be independent of W and z within the measurement errors and amounts to 8.05 +- 0.06 stat +- 0.89 syst mub on average. The data are well described by a Triple Regge model in which the process is mediated by a mixture of exchanges with an effective Regge trajectory of intercept alpha_i(0)=0.33 +- 0.04 stat +- 0.04 syst. The total cross section for the interaction of the photon with this mixture (gamma alpha_i -> X) can be described by an effective trajectory of intercept alpha_k(0)=0.99 +- 0.01 stat +- 0.05 syst. Predictions based on previous triple Regge analyses of pp-> pX data assuming vertex factorisation are broadly consistent with the gamma p data. The measured cross sections are compared with deep inelastic scattering leading proton data in the same region of z and pT_proton for photon virtuality Q^2 > 2.5 GeV^2. The ratio of the cross section for leading proton production to the total cross section is found to rise with Q^2.<br />17 pages, 6 figures, 1 table, analysis has been extended by comparison with pp data

Details

Language :
English
ISSN :
05503213
Database :
OpenAIRE
Journal :
Nuclear Physics B, Nuclear Physics B, Elsevier, 2001, 619, pp.3-21, Nuclear physics : B, ResearcherID, Nuclear Physics B, 2001, 619, pp.3-21
Accession number :
edsair.doi.dedup.....b6cbe376341a7ad82ef178a8d4df7b59