Proton and antiproton distributions at midrapidity in proton-nucleus and sulphur-nucleus collisions

被引:26
作者
Bearden, IG [1 ]
Boggild, H
Boissevain, J
Dodd, J
Esumi, S
Fabjan, CW
Fields, DE
Franz, A
Hansen, AG
Holzer, EB
Humanic, TJ
Jacak, BV
Jayanti, R
Kalechofsky, H
Lee, YY
Leltchouk, M
Lorstad, B
Maeda, N
Medvedv, A
Miyabayashi, A
Murray, M
Nishimura, S
Pandey, SU
Piuz, F
Polychronakos, V
Potekhin, M
Poulard, G
Sakaguchi, A
Sarabura, M
Spegel, M
Simon-Gillo, J
Sondheim, W
Sugitate, T
Sullivan, JP
Sumi, Y
van Hecke, H
Willis, WJ
Wolf, K
Xu, N
机构
[1] Niels Bohr Inst, DK-2100 Copenhagen, Denmark
[2] Los Alamos Natl Lab, Los Alamos, NM USA
[3] Columbia Univ, New York, NY 10027 USA
[4] Hiroshima Univ, Higashihiroshima 724, Japan
[5] CERN, CH-1211 Geneva 23, Switzerland
[6] Ohio State Univ, Columbus, OH 43210 USA
[7] Univ Pittsburgh, Pittsburgh, PA 15260 USA
[8] Lund Univ, S-22362 Lund, Sweden
[9] Texas A&M Univ, College Stn, TX 77843 USA
[10] Brookhaven Natl Lab, Upton, NY 11973 USA
来源
PHYSICAL REVIEW C | 1998年 / 57卷 / 02期
关键词
D O I
10.1103/PhysRevC.57.837
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
Experiment NA44 has measured proton and antiproton distributions at midrapidity in sulphur and proton collisions with nuclear targets at 200 and 450 GeV/c per nucleon respectively. The inverse slopes of transverse mass distributions increase with system size for both protons and antiprotons but are slightly lower for antiprotons. This could happen if antiprotons are annihilated in the nuclear medium. The antiproton yield increases with system size and centrality and is largest at midrapidity. The proton yield also increases with system size and centrality, but decreases from backward rapidity to midrapidity. The stopping of protons at these energies lies between the full stopping and nuclear transparency scenarios. The data are in reasonable agreement with RQMD predictions except for the antiproton yields from sulphur-nucleus collisions.
引用
收藏
页码:837 / 846
页数:10
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