The Q2 dependence of dijet cross sections in γp interactions at HERA

被引:24
作者
Breitweg, J
Chekanov, S
Derrick, M
Krakauer, D
Magill, S
Musgrave, B
Pellegrino, A
Repond, J
Stanek, R
Yoshida, R
Mattingly, MCK
Abbiendi, G
Anselmo, F
Antonioli, P
Bari, G
Basile, M
Bellagamba, L
Boscherini, D
Bruni, A
Bruni, G
Romeo, GC
Castellini, G
Cifarelli, L
Cindolo, F
Contin, A
Coppola, N
Corradi, M
De Pasquale, S
Giusti, P
Iacobucci, G
Laurenti, G
Levi, G
Margotti, A
Massam, T
Nania, R
Palmonari, F
Pesci, A
Polini, A
Sartorelli, G
Garcia, YZ
Zichichi, A
Amelung, C
Bornheim, A
Brock, I
Coböken, K
Crittenden, J
Deffner, R
Hartmann, H
Heinloth, K
Hilger, E
机构
[1] Argonne Natl Lab, Argonne, IL 60439 USA
[2] Andrews Univ, Berrien Springs, MI 49104 USA
[3] Univ Bologna, Bologna, Italy
[4] Ist Nazl Fis Nucl, I-40126 Bologna, Italy
[5] Univ Bonn, Inst Phys, D-5300 Bonn, Germany
[6] Univ Bristol, HH Wills Phys Lab, Bristol BS8 1TL, Avon, England
[7] Univ Calabria, Dept Phys, I-87036 Cosenza, Italy
[8] Ist Nazl Fis Nucl, Cosenza, Italy
[9] Chonnam Natl Univ, Kwangju 500757, South Korea
[10] Columbia Univ, Nevis Labs, Irvington, NY USA
[11] Inst Nucl Phys, Krakow, Poland
[12] Acad Min & Met, Fac Phys & Nucl Techniques, Krakow, Poland
[13] Jagiellonian Univ, Dept Phys, Krakow, Poland
[14] Deutsch Elekt Synchrotron DESY, Hamburg, Germany
[15] DESY Zeuthen, Zeuthen, Germany
[16] Univ Florence, Florence, Italy
[17] Ist Nazl Fis Nucl, I-50125 Florence, Italy
[18] Ist Nazl Fis Nucl, Lab Nazl Frascati, I-00044 Frascati, Italy
[19] Univ Freiburg, Fak Phys, D-7800 Freiburg, Germany
[20] Univ Glasgow, Dept Phys & Astron, Glasgow, Lanark, Scotland
[21] Univ Hamburg, Inst Expt Phys 1, Hamburg, Germany
[22] Univ Hamburg, Inst Expt Phys 2, D-2000 Hamburg, Germany
[23] Univ London Imperial Coll Sci Technol & Med, High Energy Nucl Phys Grp, London, England
[24] Univ Iowa, Dept Phys & Astron, Iowa City, IA 52242 USA
[25] Forschungszentrum Julich, Inst Kernphys, Julich, Germany
[26] KEK, Inst Particle & Nucl Studies, Tsukuba, Ibaraki, Japan
[27] Korea Univ, Seoul 136701, South Korea
[28] Kyungpook Natl Univ, Taegu 702701, South Korea
[29] Univ Autonoma Madrid, Dept Fis Teor, Madrid, Spain
[30] McGill Univ, Dept Phys, Montreal, PQ, Canada
[31] Meiji Gakuin Univ, Fac Gen Educ, Yokohama, Kanagawa, Japan
[32] Moscow Engn Phys Inst, Moscow 115409, Russia
[33] Moscow MV Lomonosov State Univ, Inst Nucl Phys, Moscow, Russia
[34] NIKHEF H, NL-1009 DB Amsterdam, Netherlands
[35] Univ Amsterdam, Amsterdam, Netherlands
[36] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
[37] Univ Oxford, Dept Phys, Oxford, England
[38] Univ Padua, Dipartimento Fis, Padua, Italy
[39] Ist Nazl Fis Nucl, Padua, Italy
[40] Penn State Univ, Dept Phys, University Pk, PA 16802 USA
[41] Polytech Univ, Sagamihara, Kanagawa, Japan
[42] Univ Roma La Sapienza, Dipartimento Fis, I-00185 Rome, Italy
[43] Ist Nazl Fis Nucl, Rome, Italy
[44] Rutherford Appleton Lab, Didcot OX11 0QX, Oxon, England
[45] Univ Calif Santa Cruz, Santa Cruz, CA 95064 USA
[46] Univ Siegen, Fachbereich Phys, D-5900 Siegen, Germany
[47] Tel Aviv Univ, Raymond & Beverly Sackler Fac Exact Sci, Sch Phys, IL-69978 Tel Aviv, Israel
[48] Univ Tokyo, Dept Phys, Tokyo 113, Japan
[49] Tokyo Metropolitan Univ, Dept Phys, Tokyo, Japan
[50] Univ Turin, Dipartimento Fis Sperimentale, Turin, Italy
关键词
D O I
10.1016/S0370-2693(00)00311-7
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The dependence of the photon structure on the photon virtuality, Q(2), is studied by measuring the reaction e(+) p --> e(+) + jet + jet + X at photon-proton centre-of-mass energies 134 < W < 223 GeV. Events have been selected in the Q(2) ranges approximate to 0 GeV2, 0.1-0.55 GeV2, and 1.5-4.5 GeV2, having two jets with transverse energy E-f(jet) > 5.5 GeV in Ihe Final state. The dijet cross section has been measured as a Function of the fractional momentum of the photon participating in the hard process, x(gamma)(OBS). The ratio of the dijet cross section with x(gamma)(OBS) < 0.75 to that with x(gamma)(OBS) > 0.75 decreases as Q(2) increases. The data are compared with the predictions of NLO pQCD and leading-order Monte Carlo programs using various parton distribution functions of the photon. The measurements can be interpreted in terms of a resolved photon component that falls with Q(2) but remains present at values of Q(2) up to 4.5 GeV2. However, none of the models considered gives a good description of the data. (C) 2000 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:37 / 52
页数:16
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