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Phys. Rev. D 79, 012001 (2009) [18 pages]

Production of the charmonium states chic1 and chic2 in proton nucleus interactions at sqrt(s)=41.6 GeV

I. Abt,24 M. Adams,11 M. Agari,14 H. Albrecht,13 A. Aleksandrov,30 V. Amaral,9 A. Amorim,9 S. J. Aplin,13 V. Aushev,17 Y. Bagaturia,13,37 V. Balagura,23 M. Bargiotti,6 O. Barsukova,12 J. Bastos,9 J. Batista,9 C. Bauer,14 Th. S. Bauer,1 A. Belkov,12 Ar. Belkov,12 I. Belotelov,12 A. Bertin,6 B. Bobchenko,23 M. Böcker,27 A. Bogatyrev,23 G. Bohm,30 M. Bräuer,14 M. Bruinsma,29,1 M. Bruschi,6 P. Buchholz,27 T. Buran,25 J. Carvalho,9 P. Conde,2,13 C. Cruse,11 M. Dam,10 K. M. Danielsen,25 M. Danilov,23 S. De Castro,6 H. Deppe,15 X. Dong,3 H. B. Dreis,15 V. Egorytchev,13 K. Ehret,11 F. Eisele,15 D. Emeliyanov,13 S. Essenov,23 L. Fabbri,6 P. Faccioli,6 M. Feuerstack-Raible,15 J. Flammer,13 B. Fominykh,23 M. Funcke,11 Ll. Garrido,2 A. Gellrich,30 B. Giacobbe,6 J. Gläß,21 D. Goloubkov,13,34 Y. Golubkov,13,35 A. Golutvin,23 I. Golutvin,12 I. Gorbounov,13,27 A. Gorišek,18 O. Gouchtchine,23 D. C. Goulart,8 S. Gradl,15 W. Gradl,15 F. Grimaldi,6 J. Groth-Jensen,10 Yu. Guilitsky,23,36 J. D. Hansen,10 J. M. Hernández,30 W. Hofmann,14 M. Hohlmann,13 T. Hott,15 W. Hulsbergen,1 U. Husemann,27 O. Igonkina,23 M. Ispiryan,16 T. Jagla,14 C. Jiang,3 H. Kapitza,13 S. Karabekyan,26 N. Karpenko,12 S. Keller,27 J. Kessler,15 F. Khasanov,23 Yu. Kiryushin,12 I. Kisel,24 E. Klinkby,10 K. T. Knöpfle,14 H. Kolanoski,5 S. Korpar,22,18 C. Krauss,15 P. Kreuzer,13,20 P. Križan,19,18 D. Krücker,5 S. Kupper,18 T. Kvaratskheliia,23 A. Lanyov,12 K. Lau,16 B. Lewendel,13 T. Lohse,5 B. Lomonosov,13,33 R. Männer,21 R. Mankel,30 S. Masciocchi,13 I. Massa,6 I. Matchikhilian,23 G. Medin,5 M. Medinnis,13 M. Mevius,13 A. Michetti,13 Yu. Mikhailov,23,36 R. Mizuk,23 R. Muresan,10 M. zur Nedden,5 M. Negodaev,13,33 M. Nörenberg,13 S. Nowak,30 M. T. Núñez Pardo de Vera,13 M. Ouchrif,29,1 F. Ould-Saada,25 C. Padilla,13 D. Peralta,2 R. Pernack,26 R. Pestotnik,18 B. AA. Petersen,10 M. Piccinini,6 M. A. Pleier,14 M. Poli,6,32 V. Popov,23 D. Pose,12,15 S. Prystupa,17 V. Pugatch,17 Y. Pylypchenko,25 J. Pyrlik,16 K. Reeves,14 D. Reßing,13 H. Rick,15 I. Riu,13 P. Robmann,31 I. Rostovtseva,23 V. Rybnikov,13 F. Sánchez,14 A. Sbrizzi,1 M. Schmelling,14 B. Schmidt,13 A. Schreiner,30 H. Schröder,26 U. Schwanke,30 A. J. Schwartz,8 A. S. Schwarz,13 B. Schwenninger,11 B. Schwingenheuer,14 F. Sciacca,14 N. Semprini-Cesari,6 S. Shuvalov,23,5 L. Silva,9 L. Sözüer,13 S. Solunin,12 A. Somov,13 S. Somov,13,34 J. Spengler,13 R. Spighi,6 A. Spiridonov,30,23 A. Stanovnik,19,18 M. Starič,18 C. Stegmann,5 H. S. Subramania,16 M. Symalla,13,11 I. Tikhomirov,23 M. Titov,23 I. Tsakov,28 U. Uwer,15 C. van Eldik,13,11 Yu. Vassiliev,17 M. Villa,6 A. Vitale,6,7 I. Vukotic,5,30 H. Wahlberg,29 A. H. Walenta,27 M. Walter,30 J. J. Wang,4 D. Wegener,11 U. Werthenbach,27 H. Wolters,9 R. Wurth,13 A. Wurz,21 S. Xella-Hansen,10 Yu. Zaitsev,23 M. Zavertyaev,13,14,33 T. Zeuner,13,27 A. Zhelezov,23 Z. Zheng,3 R. Zimmermann,26 T. Živko,18 and A. Zoccoli6

(HERA-B Collaboration)

1NIKHEF, 1009 DB Amsterdam, The Netherlands
2Department ECM, Faculty of Physics, University of Barcelona, E-08028 Barcelona, Spain
3Institute for High Energy Physics, Beijing 100039, P.R. China
4Institute of Engineering Physics, Tsinghua University, Beijing 100084, P.R. China
5Institut für Physik, Humboldt-Universität zu Berlin, D-12489 Berlin, Germany
6Dipartimento di Fisica dell' Università di Bologna and INFN Sezione di Bologna, I-40126 Bologna, Italy
7Fondazione Giuseppe Occhialini, I-61034 Fossombrone (Pesaro Urbino), Italy
8Department of Physics, University of Cincinnati, Cincinnati, Ohio 45221, USA
9LIP Coimbra, P-3004-516 Coimbra, Portugal
10Niels Bohr Institutet, DK 2100 Copenhagen, Denmark
11Institut für Physik, Universität Dortmund, D-44221 Dortmund, Germany
12Joint Institute for Nuclear Research Dubna, 141980 Dubna, Moscow, Russia
13DESY, D-22603 Hamburg, Germany
14Max-Planck-Institut für Kernphysik, D-69117 Heidelberg, Germany
15Physikalisches Institut, Universität Heidelberg, D-69120 Heidelberg, Germany
16Department of Physics, University of Houston, Houston, Texas 77204, USA
17Institute for Nuclear Research, Ukrainian Academy of Science, 03680 Kiev, Ukraine
18J. Stefan Institute, 1001 Ljubljana, Slovenia
19University of Ljubljana, 1001 Ljubljana, Slovenia
20University of California, Los Angeles, California 90024, USA
21Lehrstuhl für Informatik V, Universität Mannheim, D-68131 Mannheim, Germany
22University of Maribor, 2000 Maribor, Slovenia
23Institute of Theoretical and Experimental Physics, 117218 Moscow, Russia
24Max-Planck-Institut für Physik, Werner-Heisenberg-Institut, D-80805 München, Germany
25Department of Physics, University of Oslo, N-0316 Oslo, Norway
26Fachbereich Physik, Universität Rostock, D-18051 Rostock, Germany
27Fachbereich Physik, Universität Siegen, D-57068 Siegen, Germany
28INRNE-BAS, Sofia, Bulgaria
29Universiteit Utrecht/NIKHEF, 3584 CB Utrecht, The Netherlands
30DESY, D-15738 Zeuthen, Germany
31Physik-Institut, Universität Zürich, CH-8057 Zürich, Switzerland
32Dipartimento di Energetica dell' Università di Firenze and INFN Sezione di Bologna, Italy
33P.N. Lebedev Physical Institute, 117924 Moscow B-333, Russia
34Moscow Physical Engineering Institute, 115409 Moscow, Russia
35Moscow State University, 119992 Moscow, Russia
36Institute for High Energy Physics, Protvino, Russia
37High Energy Physics Institute, 380086 Tbilisi, Georgia

Received 14 July 2008; published 13 January 2009

A measurement of the ratio Rchic=(chic-->J/psi+gamma)/J/psi in pC, pTi, and pW interactions at 920 GeV/c (sqrt(s)=41.6 GeV) in the Feynman-x range -0.35<xFJ/psi<0.15 is presented. Both µ+µ- and e+e- J/psi decay channels are observed with an overall statistics of about 15 000 chic events, which is by far the largest available sample in pA collisions. The result is Rchic=0.188±0.013st((+0.024)/(-0.022))sys averaged over the different materials, when no J/psi and chic polarizations are considered. The chic1 to chic2 production ratio R12=Rchic1/Rchic2 is measured to be 1.02±0.40, leading to a cross section ratio ((sigma(chi[sub c1]))/(sigma(chi[sub c2])))=0.57±0.23. The dependence of Rchic on the Feynman-x of the J/psi, xFJ/psi, and its transverse momentum, pTJ/psi, is studied, as well as its dependence on the atomic number, A, of the target. For the first time, an extensive study of possible biases on Rchic and R12 due to the dependence of acceptance on the polarization states of J/psi and chic is performed. By varying the polarization parameter, lambdaobs, of all produced J/psi's by two sigma around the value measured by HERA-B, and considering the maximum variation due to the possible chic1 and chic2 polarizations, it is shown that Rchic could change by a factor between 1.02 and 1.21 and R12 by a factor between 0.89 and 1.16.

©2009 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevD.79.012001
DOI: 10.1103/PhysRevD.79.012001
PACS: 13.20.Gd; 13.85.-t; 24.85.+p; 13.88.+e
  • 13.20.Gd
    Leptonic/semileptonic/radiative decays of J/ψ, Υ, and other quarkonia
  • 13.85.-t
    Hadron-induced high- and super-high-energy interactions (energy>10 GeV)
  • 24.85.+p
    Quarks, gluons and QCD in nuclear reactions
  • 13.88.+e
    Polarization in elementary particle interactions and scattering
  • YEAR: 2008

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