Measurement and QCD analysis of the diffractive deep-inelastic scattering cross section at HERA

被引:250
|
作者
Aktas, 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.
Buesser, 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.
Coppens, Y. R.
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.
机构
[1] DESY, D-2000 Hamburg, Germany
[2] Rhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, Germany
[3] Univ Birmingham, Sch Phys & Astron, Birmingham, W Midlands, England
[4] Inter Univ Inst High Energies ULB VUB, Brussels, Belgium
[5] Univ Antwerp, B-2020 Antwerp, Belgium
[6] Rutherford Appleton Lab, Chilton, Didcot, England
[7] Inst Nucl Phys, Krakow, Poland
[8] Univ Dortmund, Inst Phys, D-4600 Dortmund, Germany
[9] Joint Inst Nucl Res, Dubna, Russia
[10] CEA, DSM, DAPNIA, CE Saclay, Gif Sur Yvette, France
[11] Univ Hamburg, Inst Expt Phys, Hamburg, Germany
[12] Max Planck Inst Kernphys, Heidelberg, Germany
[13] Heidelberg Univ, Inst Phys, D-6900 Heidelberg, Germany
[14] Heidelberg Univ, Kirchoff Inst Phys, Heidelberg, Germany
[15] Univ Kiel, Inst Expt & Angew Phys, Kiel, Germany
[16] Slovak Acad Sci, Inst Expt Phys, Kosice 04353, Slovakia
[17] Univ Lancaster, Dept Phys, Lancaster, England
[18] Univ Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, England
[19] Queen Mary Univ London, London E1 4NS, England
[20] Lund Univ, Dept Phys, Lund, Sweden
[21] Univ Manchester, Dept Phys, Manchester M13 9PL, Lancs, England
[22] Univ Aix Marseille 2, CPPM, CNRS, IN2P3, Marseille, France
[23] CINVESTAV, Dept Fis Aplicada, Merida, Yucatan, Mexico
[24] CINVESTAV, Dept Fis, Merida, Yucatan, Mexico
[25] Inst Theoret & Expt Phys, Moscow 117259, Russia
[26] PN Lebedev Phys Inst, Moscow 117924, Russia
[27] Max Planck Inst Phys & Astrophys, D-80805 Munich, Germany
[28] Univ Paris Sud 11, LAL, IN2P3, CNRS, Orsay, France
[29] Ecole Polytech, LLR, IN2P3, CNRS, Palaiseau, France
[30] Univ Paris 06, LPNHE, Paris, France
[31] Univ Paris 07, IN2P3, CNRS, Paris, France
[32] Univ Montenegro, Fac Sci, Podgorica, Montenegro
[33] Acad Sci Czech Republic, Inst Phys, Prague, Czech Republic
[34] Charles Univ Prague, Fac Math & Phys, Prague, Czech Republic
[35] Univ Roma Tre, Dipartmento Fis, Rome, Italy
[36] INFN Roma 3, Rome, Italy
[37] Inst Nucl Energy Res, Sofia, Bulgaria
[38] Paul Scherrer Inst, Villigen, Switzerland
[39] Univ Wuppertal, Fachbereich C, Wuppertal, Germany
[40] Yerevan Phys Inst, Yerevan, Armenia
[41] DESY, Zeuthen, Germany
[42] ETH, Inst Teilchenphys, Zurich, Switzerland
[43] Univ Zurich, Inst Phys, Zurich, Switzerland
[44] Natl Tech Univ Athens, Dept Phys, Athens 15773, Greece
[45] Univ Wuppertal, Rechenzentrum, Wuppertal, Germany
[46] Safarik Univ, Kosice, Slovakia
[47] CERN, Geneva, Switzerland
[48] Max Planck Inst Phys & Astrophys, D-80805 Munich, Germany
[49] Comenius Univ, Bratislava, Slovakia
[50] Univ Antwerp, Phys Dept, Antwerp, Belgium
来源
EUROPEAN PHYSICAL JOURNAL C | 2006年 / 48卷 / 03期
基金
英国科学技术设施理事会;
关键词
D O I
10.1140/epjc/s10052-006-0035-3
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
A detailed analysis is presented of the diffractive deep-inelastic scattering process ep -> eXY, where Y is a proton or a low mass proton excitation carrying a fraction 1 - x(IP) > 0.95 of the incident proton longitudinal momentum and the squared four-momentum transfer at the proton vertex satisfies |t| < 1 GeV2. Using data taken by the H1 experiment, the cross section is measured for photon virtualities in the range 3.5 <= Q(2) <= 1600 GeV2, triple differentially in x(IP), Q(2) and beta = x/x(P), where x is the Bjorken scaling variable. At low x(IP), the data are consistent with a factorisable x(IP) dependence, which can be described by the exchange of an effective pomeron trajectory with intercept alpha(IP)(0) = 1.118 +/- 0.008(exp.)(-0.010)(+0.029)(model). Diffractive parton distribution functions and their uncertainties are determined from a next-to-leading order DGLAP QCD analysis of the Q(2)and beta dependences of the cross section. The resulting gluon distribution carries an integrated fraction of around 70% of the exchanged momentum in the Q(2) range studied. Total and differential cross sections are also measured for the diffractive charged current process e(+) p -> (v) over bar eXY and are found to be well described by predictions based on the diffractive parton distributions. The ratio of the diffractive to the inclusive neutral current ep cross sections is studied. Over most of the kinematic range, this ratio shows no significant dependence on Q(2) at fixed x(P) and x or on x at fixed Q(2) and beta.
引用
收藏
页码:715 / 748
页数:34
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