Summary
We attempt to provide an explanation to the charged-particle multiplicity distributions in oxygen-nucleus collision at 60 and 200 GeV per nucleon obtained from Helios Collaboration which is based on an earlier work done onE T distributions. The differences between transverse energy (E T) distribution and multiplicity distributions will also be elucidated.
Similar content being viewed by others
References
Helios Collaboration (T. Akesson et al.):Nucl. Phys. B,333, 48 (1990).
Helios Collaboration (T. Akesson et al.):Phys. Lett. B,214, 295 (1988).
Helios Collaboration (T. Akesson et al.):Z. Phys. C,38, 383 (1988).
NA35Collaboration (A. Barnberger et al.):Phys. Lett. B,205, 583 (1988).
G. Baym et al.:Phys. Lett. B,190, 29 (1987).A. D. Jackson andH. Boggild:Nucl. Phys. A,470, 669 (1987).
Chao Wei-qin andLiu Bo:Z. Phys. C,42, 337 (1989).
A. H. Chan andC. K. Chew:Nuovo Cimento A,104, 81 (1991).
C. K. Chew:Phys. Lett. B,186, 411 (1987).
A. H. Chan andC. K. Chew:Phys. Rev. D,41, 851 (1990).
K. Konishi et al.:Nucl. Phys. B,157, 45 (1979).
A. Giovannini:Nucl. Phys. B,161, 429 (1979).
W. Thomé et al.:Nucl. Phys. B,129, 365 (1977).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Chan, A.H., Chew, C.K. A generalized multiplicity distribution for high-energy nucleus-nucleus collisions. Nuov Cim A 105, 941–948 (1992). https://doi.org/10.1007/BF02730835
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02730835