Charged particle production in proton-, deuteron-, oxygen- and sulphur-nucleus collisions at 200 GeV per nucleon

The NA35 Collaboration:     T. Alber - et al.

doi:doi:10.1007/s100529800867

2018 Impact factor 4.843

Particles and Fields

Eur. Phys. J. C 2, 643-659
DOI 10.1007/s100529800867

Charged particle production in proton-, deuteron-, oxygen-
and sulphur-nucleus collisions at 200 GeV per nucleon

The NA35 Collaboration:
T. Alber¹⁰ - H. Appelshäuser⁶ - J. Bächler⁵ - J. Bartke⁴ - H. Bia $\l$ kowska¹² - M.A. Bloomer³ - R. Bock⁵ - W.J. Braithwaite¹⁰ - D. Brinkmann⁶ - R. Brockmann⁵ - P. Buncic⁵ - P. Chan¹⁰ - J.G. Cramer¹⁰ - P.B. Cramer¹⁰ - I. Derado⁹ - B. Eberlein⁶ - V. Eckardt⁹ - J. Eschke⁶ - C. Favuzzi² - D. Ferenc¹³ - B. Fleischmann⁵ - P. Foka⁵ - P. Freund⁹ - M. Fuchs⁶ - M. Gazdzicki⁶ - E. G $\l$ adysz⁴ - J. Grebieszkow¹¹ - J. Günther⁶ - J.W. Harris³ - M. Hoffmann⁷ - P. Jacobs³ - S. Kabana⁶ - K. Kadija^9,13 - R. Keidel⁸ - M. Kowalski⁴ - A. Kühmichel⁶ - F. Lave⁶ - J.Y. Lee⁶ - A. Ljubicic jr.¹³ - S. Margetis³ - J.T. Mitchell³ - R. Morse³ - E. Nappi² - G. Odyniec³ - G. Paic^5,13 - A.D. Panagiotou¹ - A. Petridis¹ - A. Piper⁸ - F. Posa² - A.M. Poskanzer³ - F. Pühlhofer⁸ - W. Rauch⁹ - R. Renfordt⁶ - W. Retyk¹¹ - D. Röhrich⁶ - G. Roland⁶ - H. Rothard⁶ - K. Runge⁷ - A. Sandoval⁵ - N. Schmitz⁹ - E. Schmoetten⁷ - R. Sendelbach⁶ - P. Seyboth⁹ - J. Seyerlein⁹ - E. Skrzypczak¹¹ - P. Spinelli² - R. Stock⁶ - H. Ströbele⁶ - L. Teitelbaum³ - S. Tonse³ - T.A. Trainor¹⁰ - G. Vasileiadis¹ - M. Vassiliou¹ - G. Vesztergombi⁹ - D. Vranic¹³ - S. Wenig⁶ - B. Wosiek^9,4 - X. Zhu¹⁰

¹ Department of Physics, University of Athens, Athens, Greece
² Dipartimento di Fisica, Università di Bari and INFN Bari, Bari, Italy
³ Lawrence Berkeley Laboratory, Berkeley, CA, USA
⁴ Institute of Nuclear Physics, Cracow, Poland
⁵ Gesellschaft für Schwerionenforschung (GSI), Darmstadt, Germany
⁶ Fachbereich Physik der Universität, Frankfurt, Germany (IKF)
⁷ Fakultät für Physik der Universität, Freiburg, Germany
⁸ Fachbereich Physik der Universität, Marburg, Germany
⁹ Max-Planck-Institut für Physik, München, Germany
¹⁰ University of Washington, Seattle, USA
¹¹ Institute for Experimental Physics, University of Warsaw, Warsaw, Poland
¹² Institute for Nuclear Studies, Warsaw, Poland
¹³ Rudjer Boskovic Institute, Zagreb

Received: 28 October 1997 / Published online: 10 March 1998

Abstract
The transverse momentum and rapidity distributions of net protons and negatively charged hadrons have been measured for minimum bias proton-nucleus and deuteron-gold interactions, as well as central oxygen-gold and sulphur-nucleus collisions at 200 GeV per nucleon. The rapidity density of net protons at midrapidity in central nucleus-nucleus collisions increases both with target mass for sulphur projectiles and with the projectile mass for a gold target. The shape of the rapidity distributions of net protons forward of midrapidity for d+Au and central S+Au collisions is similar. The average rapidity loss is larger than 2 units of rapidity for reactions with the gold target. The transverse momentum spectra of net protons for all reactions can be described by a thermal distribution with `temperatures' between $145 \pm 11$ MeV (p+S interactions) and $244 \pm 43$ MeV (central S+Au collisions). The multiplicity of negatively charged hadrons increases with the mass of the colliding system. The shape of the transverse momentum spectra of negatively charged hadrons changes from minimum bias p+p and p+S interactions to p+Au and central nucleus-nucleus collisions. The mean transverse momentum is almost constant in the vicinity of midrapidity and shows little variation with the target and projectile masses. The average number of produced negatively charged hadrons per participant baryon increases slightly from p+p, p+A to central S+S,Ag collisions.