Table 32
View DatasetAktas, A.;Andreev, V.;Anthonis, T.;Antunovic, B.;Aplin, S.;Asmone, A.;Astvatsatourov, A.;Babaev, A.;Backovic, S.;Baghdasaryan, A.;Baranov, P.;Barrelet, E.;Bartel, W.;Baudrand, S.;Baumgartner, S.;Beckingham, M.;Behnke, O.;Behrendt, O.;Belousov, A.;Berger, N.;Bizot, J.C.;Boenig, M.-O.;Boudry, V.;Bracinik, J.;Brandt, G.;Brisson, V.;Bruncko, D.;Busser, F.W.;Bunyatyan, A.;Buschhorn, G.;Bystritskaya, L.;Campbell, A.J.;Cassol-Brunner, F.;Cerny, K.;Cerny, V.;Chekelian, V.;Contreras, J.G.;Coughlan, J.A.;Cox, B.E.;Cozzika, G.;Cvach, J.;Dainton, J.B.;Dau, W.D.;Daum, K.;De Boer, Y.;Delcourt, B.;Del Degan, M.;De Roeck, A.;De Wolf, E.A.;Diaconu, C.;Dodonov, V.;Dubak, A.;Eckerlin, Guenter;Efremenko, V.;Egli, S.;Eichler, R.;Eisele, F.;Eliseev, A.;Elsen, E.;Essenov, S.;Falkewicz, A.;Faulkner, P.J.W.;Favart, L.;Fedotov, A.;Felst, R.;Feltesse, J.;Ferencei, J.;Finke, L.;Fleischer, M.;Flucke, G.;Fomenko, A.;Franke, G.;Frisson, T.;Gabathuler, E.;Garutti, E.;Gayler, J.;Gerlich, C.;Ghazaryan, Samvel;Ginzburgskaya, S.;Glazov, A.;Glushkov, I.;Goerlich, L.;Goettlich, M.;Gogitidze, N.;Gorbounov, S.;Grab, C.;Greenshaw, T.;Gregori, M.;Grell, B.R.;Grindhammer, G.;Gwilliam, C.;Haidt, D.;Hansson, M.;Heinzelmann, G.;Henderson, R.C.W.;Henschel, H.;Herrera, G.;Hildebrandt, M.;Hiller, K.H.;Hoffmann, D.;Horisberger, R.;Hovhannisyan, A.;Hreus, T.;Hussain, S.;Ibbotson, M.;Ismail, M.;Jacquet, M.;Janssen, X.;Jemanov, V.;Jonsson, L.;Johnson, D.P.;Jung, Andreas Werner;Jung, H.;Kapichine, M.;Katzy, J.;Kenyon, I.R.;Kiesling, Christian M.;Klein, M.;Kleinwort, C.;Klimkovich, T.;Kluge, T.;Knies, G.;Knutsson, A.;Korbel, V.;Kostka, P.;Krastev, K.;Kretzschmar, J.;Kropivnitskaya, A.;Kruger, K.;Landon, M.P.J.;Lange, W.;Lastovicka-Medin, G.;Laycock, P.;Lebedev, A.;Leibenguth, G.;Lendermann, V.;Levonian, S.;Lindfeld, L.;Lipka, K.;Liptaj, A.;List, B.;List, J.;Lobodzinska, E.;Loktionova, N.;Lopez-Fernandez, R.;Lubimov, V.;Lucaci-Timoce, A.-I.;Lueders, H.;Lux, T.;Lytkin, L.;Makankine, A.;Malden, N.;Malinovski, E.;Marage, P.;Marshall, R.;Marti, L.;Martisikova, M.;Martyn, H.-U.;Maxfield, S.J.;Mehta, A.;Meier, K.;Meyer, A.B.;Meyer, H.;Meyer, J.;Michels, V.;Mikocki, S.;Milcewicz-Mika, I.;Milstead, D.;Mladenov, D.;Mohamed, A.;Moreau, F.;Morozov, A.;Morris, J.V.;Mozer, Matthias Ulrich;Muller, K.;Murin, P.;Nankov, K.;Naroska, B.;Naumann, Th.;Newman, Paul R.;Niebuhr, C.;Nikiforov, A.;Nowak, G.;Nowak, K.;Nozicka, M.;Oganezov, R.;Olivier, B.;Olsson, J.E.;Osman, S.;Ozerov, D.;Palichik, V.;Panagoulias, I.;Papadopoulou, T.;Pascaud, C.;Patel, G.D.;Peng, H.;Perez, E.;Perez-Astudillo, D.;Perieanu, A.;Petrukhin, A.;Pitzl, D.;Placakyte, R.;Portheault, B.;Povh, B.;Prideaux, P.;Rahmat, A.J.;Raicevic, N.;Reimer, P.;Rimmer, A.;Risler, C.;Rizvi, E.;Robmann, P.;Roland, B.;Roosen, R.;Rostovtsev, A.;Rurikova, Z.;Rusakov, S.;Salvaire, F.;Sankey, D.P.C.;Sauter, M.;Sauvan, E.;Schilling, F.-P.;Schmidt, S.;Schmitt, S.;Schmitz, C.;Schoeffel, L.;Schoning, A.;Schultz-Coulon, H.-C.;Sefkow, F.;Shaw-West, R.N.;Sheviakov, I.;Shtarkov, L.N.;Sloan, T.;Smirnov, P.;Soloviev, Y.;South, D.;Spaskov, V.;Specka, Arnd E.;Steder, M.;Stella, B.;Stiewe, J.;Stoilov, A.;Straumann, U.;Sunar, D.;Tchoulakov, V.;Thompson, G.;Thompson, P.D.;Toll, T.;Tomasz, F.;Traynor, D.;Trinh, T.N.;Truol, P.;Tsakov, I.;Tsipolitis, G.;Tsurin, I.;Turnau, J.;Tzamariudaki, E.;Urban, K.;Urban, Marcel;Usik, A.;Utkin, D.;Valkarova, A.;Vallee, C.;Van Mechelen, P.;Vargas Trevino, A.;Vazdik, Y.;Veelken, C.;Vinokurova, S.;Volchinski, V.;Wacker, K.;Weber, G.;Weber, R.;Wegener, D.;Werner, C.;Wessels, M.;Wessling, B.;Wissing, Ch.;Wolf, R.;Wunsch, E.;Xella, S.;Yan, W.;Yeganov, V.;Zacek, J.;Zalesak, J.;Zhang, Z.;Zhelezov, A.;Zhokin, A.;Zhu, Y.C.;Zimmermann, J.;Zimmermann, T.;Zohrabyan, H.;Zomer, F.
Description
DESY-HERA. Measurement of the cross section for the diffractive DIS processE P --& gt; E X P. The data were taken during the years 1999 and 2000 with E+ and E - of energy 27.6 GeV colliding with protons of energy 920 GeV corresponding to acentre-of-mass energy of 319 GeV and have a total integrated luminosity of 28.4 pb-1. Variables used in the analysis include X(NAME=POMERON) equal to 1 - (scattered leading proton energy/ initial proton energy), and BETA equal to X/X(NAME=POMERON). Data on the T distributions and reduced cross sections (D3 and D4) are presented as functions of Q**2, X(NAME=POEMERON), BETA, and T.. Numerical values supplied by M Kapishin.
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Publication Details
Subfield
Modeling and Simulation
Field
Mathematics
Domain
Physical Sciences
Confidence Score
34%
Source
Scholar Data Model
Keywords
E- P --> E- DD PE+ P --> E+ DD PD4SIG/DBETA/DQ**2/DX/DTSIGExclusiveIntegrated Cross SectionCross SectionDiffractiveElectron productionDeep Inelastic Scattering318.0