Deep Inelastic Scattering with Leading Protons or Large Rapidity Gaps at HERA

Chekanov, S[ 1 ]; Derrick, M[ 1 ]; Magill, S[ 1 ]; Musgrave, B[ 1 ]; Nicholass, D[ 1 ]; Repond, J[ 1 ]; Yoshida, R[ 1 ]; Mattingly, MCK[ 2 ]; Antonioli, P[ 3 ]; Bari, G[ 3 ]; Bellagamba, L[ 3 ]; Boscherini, D[ 3 ]; Bruni, A[ 3 ]; Bruni, G[ 3 ]; Romeo, GC[ 3 ]; Cindolo, F[ 3 ]; Corradi, M[ 3 ]; Iacobucci, G[ 3 ]; Margotti, A[ 3 ]; Massam, T[ 3 ]; Nania, R[ 3 ]; Polini, A[ 3 ]; Antonelli,; 3, S[; 4 ], Basile; 3, M[; 4 ], Bindi; 3, M[; 4 ], Cifarelli; 3, L[; 4 ], Contin; 3, A[; 4 ], Palmonari; 3, F[; ], 4; DE PASQUALE, Salvatore; 3, S[; 4 ], Sartorelli; 3, G[; 4 ], Zichichi; 3, A[; ], 4; Bartsch, D[ 5 ]; Brock, I[ 5 ]; Hartmann, H[ 5 ]; Hilger, E[ 5 ]; Jakob, HP[ 5 ]; Jungst, M[ 5 ]; Nuncio Quiroz, AE[ 5 ]; Paul, E[ 5 ]; Samson, U[ 5 ]; Schonberg, V[ 5 ]; Shehzadi, R[ 5 ]; Wlasenko, M[ 5 ]; Brook, NH[ 6 ]; Heath, GP[ 6 ]; Morris, JD[ 6 ]; Kaur, M[ 7 ]; Kaur,; 7, P[; ], 62; Singh,; 7, I[; ], 62; Capua,; 8, M[; 9 ], Fazio; 8, S[; 9 ], Mastroberardino; 8, A[; 9 ], Schioppa; 8, M[; 9 ], Susinno; 8, G[; 9 ], Tassi; 8, E[; ], 9; Kim, JY[ 10 ]; Ibrahim, ZA[ 11 ]; Idris, FM[ 11 ]; Kamaluddin, B[ 11 ]; Abdullah, WATW[ 11 ]; Ning, Y[ 12 ]; Ren, Z[ 12 ]; Sciulli, R[ 12 ]; Chwastowski, J[ 13 ]; Eskreys, A[ 13 ]; Figiel, J[ 13 ]; Galas, A[ 13 ]; Olkiewicz, K[ 13 ]; Pawlik, B[ 13 ]; Stopa, P[ 13 ]; Zawiejski, L[ 13 ]; Adamczyk, L[ 14 ]; Bold, T[ 14 ]; Grabowska Bold, I[ 14 ]; Kisielewska, D[ 14 ]; Lukasik, J[ 14 ]; Przybycien, M[ 14 ]; Suszycki, L[ 14 ]; Kotanski, A[ 15 ]; Slominski, W[ 15 ]; Behnke, O[ 16 ]; Behrens, U[ 16 ]; Blohm, C[ 16 ]; Bonato, A[ 16 ]; Borras, K[ 16 ]; Bot, D[ 16 ]; Ciesielski, R[ 16 ]; Coppola, N[ 16 ]; Fang, S[ 16 ]; Fourletova, J[ 16 ]; Geiser, A[ 16 ]; Gottlicher, P[ 16 ]; Grebenyuk, J[ 16 ]; Gregor, I[ 16 ]; Haas, T[ 16 ]; Hain, W[ 16 ]; Huttmann, A[ 16 ]; Januschek, F[ 16 ]; Kahle, B[ 16 ]; Katkov, II[ 16 ]; Klein, U[ 16 ]; Kotz, U[ 16 ]; Kowalski, H[ 16 ]; Lisovyi, M[ 16 ]; Lobodzinska, E[ 16 ]; Lohr, B[ 16 ]; Mankel, R[ 16 ]; Melzer Pellmann, IA[ 16 ]; Miglioranzi, S[ 16 ]; 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Yamazaki, Y[ 25 ]; Barakbaev, AN[ 26 ]; Boos, EG[ 26 ]; Pokrovskiy, NS[ 26 ]; Zhautykov, BO[ 26 ]; Aushev, V[ 27 ]; Bachynska, O[ 27 ]; Borodin, M[ 27 ]; Kadenko, I[ 27 ]; Kozulia, A[ 27 ]; Libov, V[ 27 ]; Lontkovskyi, D[ 27 ]; Makarenko, I[ 27 ]; Sorokin, I[ 27 ]; Verbytskyi, A[ 27 ]; Volynets, O[ 27 ]; Son, D[ 28 ]; de Favereau, J[ 29 ]; Piotrzkowski, K[ 29 ]; Barreiro, F[ 30 ]; Glasman, C[ 30 ]; Jimenez, M[ 30 ]; Labarga, L[ 30 ]; del Peso, J[ 30 ]; Ron, E[ 30 ]; Soares, M[ 30 ]; Terron, J[ 30 ]; Uribe Estrada, C[ 30 ]; Zambrana, M[ 30 ]; Corriveau, F[ 31 ]; Liu, C[ 31 ]; Schwartz, J[ 31 ]; Walsh, R[ 31 ]; Zhou, C[ 31 ]; Tsurugai, T[ 32 ]; Antonov, A[ 33 ]; Dolgoshein, BA[ 33 ]; Gladkov, D[ 33 ]; Sosnovtsev, V[ 33 ]; Stifutkin, A[ 33 ]; Suchkov, S[ 33 ]; Dementiev, RK[ 34 ]; Ermolov, PF[ 34 ]; Gladilin, LK[ 34 ]; Golubkov, YA[ 34 ]; Khein, LA[ 34 ]; Korzhavina, IA[ 34 ]; Kuzmin, VA[ 34 ]; Levchenko, BB[ 34 ]; Lukina, OY[ 34 ]; Proskuryakov, AS[ 34 ]; Shcheglova, LM[ 34 ]; Zotkin, DS[ 34 ]; Abt, I[ 35 ]; Caldwell, A[ 35 ]; Kollar, D[ 35 ]; Reisert, B[ 35 ]; Schmidke, WB[ 35 ]; Grigorescu,; 36, G[; ], 37; Keramidas,; 36, A[; ], 37; Koffeman,; 36, E[; ], 37; Kooijman,; 36, P[; ], 37; Pellegrino,; 36, A[; ], 37; Tiecke,; 36, H[; ], 37; Vazquez,; 36, M[; ], 37; Wiggers,; 36, L[; ], 37; Brummer, N[ 38 ]; Bylsma, B[ 38 ]; Durkin, LS[ 38 ]; Lee, A[ 38 ]; Ling, TY[ 38 ]; Allfrey, PD[ 39 ]; Bell, MA[ 39 ]; Cooper Sarkar, AM[ 39 ]; Devenish, RCE[ 39 ]; Ferrando, J[ 39 ]; Foster, B[ 39 ]; Gwenlan, C[ 39 ]; Horton, K[ 39 ]; Oliver, K[ 39 ]; Robertson, A[ 39 ]; Walczak, R[ 39 ]; Bertolin, A[ 40 ]; Dal Corso, F[ 40 ]; Dusini, S[ 40 ]; Longhin, A[ 40 ]; Stanco, L[ 40 ]; Bellan,; 40, P[; ], 41; Brugnera,; 40, R[; ], 41; Carlin,; 40, R[; ], 41; Garfagnini,; 40, A[; ], 41; Limentani,; 40, S[; ], 41; BY[ 42 ], Oh; Raval, A[ 42 ]; Whitmore, JJ[ 42 ]; Iga, Y[ 43 ]; D'Agostini,; 44, G[; ], 45; Marini,; 44, G[; ], 45; Nigro,; 44, A[; ], 45; Cole, JE[ 46 ]; Hart, JC[ 46 ]; Heusch, C[ 47 ]; Sadrozinski, H[ 47 ]; 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Adamus, M[ 58 ]; Plucinski, P[ 58 ]; Ukleja, A[ 58 ]; Eisenberg, Y[ 59 ]; Hochman, D[ 59 ]; Karshon, U[ 59 ]; Brownson, E[ 60 ]; Reeder, DD[ 60 ]; Savin, AA[ 60 ]; Smith, WH[ 60 ]; Wolfe, H[ 60 ]; Bhadra, S[ 61 ]; Catterall, CD[ 61 ]; Cui, Y[ 61 ]; Hartner, G[ 61 ]; Menary, S[ 61 ]; Noor, U[ 61 ]; Standage, J[ 61 ]; Whyte, J.

doi:10.1016/j.nuclphysb.2009.03.003

The dissociation of virtual photons, γ{star operator} p → X p, in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q2 > 2 GeV2 and γ{star operator} p centre-of-mass energies 40 < W < 240 GeV, with MX > 2 GeV, where MX is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Φ, the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q2 and xP, the fraction of the proton's momentum carried by the diffractive exchange, as well as β, the Bjorken variable defined with respect to the diffractive exchange.