Leading neutron production in $\mathrm{e^+ p}$ collisions at HERA
Author(s)
Chekanov, S.Krakauer, D.
Basile, M.
Bauerdick, L. A. T.
Behrens, U.
Borras, K.
Chiochia, V.
Dannheim, D.
Derrick, M.
Drews, G.
Fourletova, J.
Fox-Murphy, A.
Fricke, U.
Bellagamba, L.
Geiser, A.
Goebel, F.
Gottlicher, P.
Gutsche, O.
Haas, Tobias M.
Hain, W.
Hartner, G. F.
Hillert, S.
Kotz, U.
Kowalski, H.
Boscherini, D.
Labes, H.
Lelas, D.
Lohr, B.
Mankel, R.
Martinez, M.
Moritz, M.
Notz, D.
Pellmann, I. A.
Petrucci, M. C.
Polini, A.
Bruni, A.
Schneekloth, U.
Selonke, F.
Surrow, B.
Wessoleck, H.
Wichmann, R.
Wolf, G.
Youngman, C.
Zeuner, W.
Lopez-Duran-Viani, Amaya
Meyer, A.
Bruni, G.
Schlenstedt, S.
Barbagli, G.
Gallo, E.
Genta, C.
Pelfer, P. G.
Bamberger, A.
Benen, A.
Coppola, N.
Markun, P.
Raach, H.
Cara Romeo, G.
Wolfle, S.
Bell, M.
Bussey, P. J.
Doyle, A. T.
Glasman, C.
Hanlon, S.
Lee, S. W.
Lupi, A.
McCance, G. J.
Saxon, D. H.
Cifarelli, L.
Skillicorn, I. O.
Gialas, I.
Bodmann, B.
Carli, T.
Holm, U.
Klimek, K.
Krumnack, N.
Lohrmann, E.
Milite, M.
Salehi, H.
Cindolo, F.
Stonjek, S.
Wick, K.
Ziegler, A.
Ziegler, Ar.
Collins-Tooth, C.
Foudas, C.
Goncalo, R.
Long, K. R.
Metlica, F.
Miller, D. B.
Contin, A.
Tapper, A. D.
Walker, R.
Cloth, P.
Filges, D.
Kuze, M.
Nagano, K.
Tokushuku, K.
Yamada, S.
Yamazaki, Y.
Barakbaev, A. N.
Corradi, M.
Boos, E. G.
Pokrovskiy, N. S.
Zhautykov, B. O.
Lim, H.
Son, D.
Barreiro, F.
Gonzalez, O.
Labarga, L.
del Peso, J.
Redondo, I.
Magill, S.
De Pasquale, S.
Terron, J.
Vazquez Acosta, Monica Luisa
Barbi, M.
Bertolin, A.
Corriveau, F.
Ochs, A.
Padhi, S.
Stairs, D. G.
St. Laurent, M.
Tsurugai, T.
Giusti, P.
Antonov, A.
Bashkirov, V.
Danilov, P.
Dolgoshein, B. A.
Gladkov, D.
Sosnovtsev, V.
Suchkov, S.
Dementiev, R. K.
Ermolov, P. F.
Golubkov, Yu. A.
Iacobucci, G.
Katkov, I. I.
Khein, L. A.
Korzhavina, I. A.
Kuzmin, V. A.
Levchenko, B. B.
Lukina, O. Yu.
Proskuryakov, A. S.
Shcheglova, L. M.
Vlasov, N. N.
Zotkin, S. A.
Levi, G.
Bokel, C.
Engelen, J.
Grijpink, S.
Koffeman, E.
Kooijman, P.
Maddox, E.
Schagen, S.
Tassi, E.
Tiecke, H.
Tuning, N.
Margotti, A.
Velthuis, J. J.
Wiggers, L.
de Wolf, E.
Brummer, N.
Bylsma, B.
Durkin, L. S.
Gilmore, J.
Ginsburg, C. M.
Kim, C. L.
Ling, T. Y.
Nania, R.
Boogert, S.
Cooper-Sarkar, Amanda M.
Devenish, R. C. E.
Ferrando, J.
Grzelak, G.
Matsushita, T.
Rigby, M.
Ruske, O.
Sutton, M. R.
Walczak, R.
Palmonari, F.
Brugnera, R.
Carlin, R.
Dal Corso, F.
Dusini, S.
Garfagnini, A.
Limentani, S.
Longhin, A.
Parenti, A.
Posocco, M.
Stanco, L.
Pesci, A.
Turcato, M.
Adamczyk, L.
Heaphy, E. A.
Oh, B. Y.
Saull, P. R. B.
Whitmore, J. J.
Iga, Y.
D'Agostini, G.
Marini, G.
Nigro, A.
Sartorelli, G.
Cormack, C.
Hart, J. C.
McCubbin, N. A.
Heusch, C.
Park, I. H.
Pavel, N.
Abramowicz, H.
Dagan, S.
Gabareen, A.
Kananov, S.
Zichichi, A.
Kreisel, A.
Levy, A.
Abe, T.
Fusayasu, T.
Kohno, T.
Umemori, K.
Yamashita, T.
Hamatsu, R.
Hirose, T.
Inuzuka, M.
Musgrave, B.
Aghuzumtsyan, G.
Kitamura, S.
Matsuzawa, K.
Nishimura, T.
Arneodo, M.
Cartiglia, N.
Cirio, R.
Costa, M.
Ferrero, M. I.
Maselli, S.
Monaco, V.
Bartsch, D.
Peroni, C.
Ruspa, M.
Sacchi, R.
Solano, A.
Staiano, A.
Fagerstroem, C. P.
Galea, R.
Koop, T.
Martin, J. F.
Mirea, A.
Brock, I.
Sabetfakhri, A.
Butterworth, J. M.
Gwenlan, C.
Hall-Wilton, R.
Jones, T. W.
Lane, J. B.
Lightwood, M. S.
Loizides, J. H.
West, B. J.
Ciborowski, J.
Crittenden, J.
Ciesielski, R.
Nowak, R. J.
Pawlak, J. M.
Smalska, B.
Sztuk, J.
Tymieniecka, T.
Ukleja, A.
Ukleja, J.
Zakrzewski, Janusz Andrzej
Zarnecki, A. F.
Goers, S.
Adamus, M.
Plucinski, P.
Eisenberg, Y.
Gladilin, L. K.
Hochman, D.
Karshon, U.
Kcira, D.
Lammers, S.
Li, L.
Reeder, D. D.
Hartmann, H.
Savin, A. A.
Smith, W. H.
Deshpande, A.
Dhawan, S.
Hughes, V. W.
Straub, P. B.
Bhadra, S.
Catterall, C. D.
Fourletov, S.
Khakzad, M.
Hilger, E.
Menary, S.
Soares, M.
Standage, J.
ZEUS Collaboration
Irrgang, P.
Jakob, H. P.
Kappes, A.
Pellegrino, A.
Katz, U. F.
Kerger, R.
Kind, O.
Paul, E.
Rautenberg, J.
Renner, R.
Schnurbusch, H.
Stifutkin, A.
Tandler, J.
Voss, K. C.
Repond, J.
Weber, A.
Bailey, D. S.
Brook, N. H.
Cole, J. E.
Foster, B.
Heath, G. P.
Heath, Helen F.
Robins, S.
Rodrigues, E.
Scott, J.
Yoshida, R.
Tapper, R. J.
Wing, M.
Capua, M.
Mastroberardino, A.
Schioppa, M.
Susinno, G.
Kim, J. Y.
Kim, Y. K.
Lee, J. H.
Lim, I. T.
Mattingly, M. C. K.
Pac, M. Y.
Caldwell, A.
Helbich, M.
Liu, X.
Mellado, B.
Paganis, S.
Schmidke, W. B.
Sciulli, F.
Chwastowski, J.
Eskreys, A.
Antonioli, P.
Figiel, J.
Olkiewicz, K.
Przybycien, M. B.
Stopa, P.
Zawiejski, L.
Bednarek, B.
Grabowska-Bold, I.
Jelen, K.
Kisielewska, D.
Kowal, A. M.
Bari, G.
Kowal, M.
Kowalski, T.
Mindur, B.
Przybycien, M.
Rulikowska-Zarebska, E.
Suszycki, L.
Szuba, D.
Szuba, J.
Kotanski, A.
Slominski, W.
Keywords
info:eu-repo/classification/ddc/530positron p: colliding beams
positron p: deep inelastic scattering
photon p: interaction
n: photoproduction
cross section: momentum transfer
x-dependence
factorization: violation
p: structure function
pi: structure function
ZEUS
experimental results
DESY HERA Stor
tables
bibliography
positron p --> n positron anything
positron p --> positron anything
approx. 300 GeV-cms
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Abstract
The production of neutrons carrying at least 20% of the proton beam energy ( x L > 0.2 ) in e + p collisions has been studied with the ZEUS detector at HERA for a wide range of Q 2 , the photon virtuality, from photoproduction to deep inelastic scattering. The neutron-tagged cross section, ep → e ′ Xn , is measured relative to the inclusive cross section, ep → e ′ X , thereby reducing the systematic uncertainties. For x L > 0.3, the rate of neutrons in photoproduction is about half of that measured in hadroproduction, which constitutes a clear breaking of factorisation. There is about a 20% rise in the neutron rate between photoproduction and deep inelastic scattering, which may be attributed to absorptive rescattering in the γp system. For 0.64< x L <0.82, the rate of neutrons is almost independent of the Bjorken scaling variable x and Q 2 . However, at lower and higher x L values, there is a clear but weak dependence on these variables, thus demonstrating the breaking of limiting fragmentation. The neutron-tagged structure function, F LN(3) 2 ( x , Q 2 , x L ), rises at low values of x in a way similar to that of the inclusive F 2 ( x , Q 2 ) of the proton. The total γπ cross section and the structure function of the pion, F π 2 ( x π , Q 2 ) where x π = x /(1− x L ), have been determined using a one-pion-exchange model, up to uncertainties in the normalisation due to the poorly understood pion flux. At fixed Q 2 , F π 2 has approximately the same x dependence as F 2 of the proton.Date
2002Type
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http://bib-pubdb1.desy.de/record/329768/files/1-s2.0-S055032130200439X-main.pdf
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