posted on 2024-08-06, 12:17authored byB. B. Back, M. D. Baker, D. S. Barton, R. R. Betts, R. Bindel, A. Budzanowski, W. Busza, A. Carroll, M. P. Decowski, E. Garcia, N. George, K. Gulbrandsen, S. Gushue, C. Halliwell, G. A. Heintzelman, C. Henderson, R. Holynski, D. J. Hofman, B. Holzman, E. Johnson, J. L. Kane, J. Katzy, N. Khan, W. Kucewicz, P. Kulinich, W. T. Lin, S. Manly, D. McLeod, J. Michalowski, A. C. Mignerey, J. Mulmenstadt, R. Nouicer, A. Olszewski, R. Pak, I. C. Park, H. Pernegger, C. Reed, L. P. Remsberg, M. Reuter, C. Roland, G. Roland, L. Rosenberg, P. Sarin, P. Sawicki, W. Skulski, S. G. Steadman, G. S. F. Stephans, P. Steinberg, M. Stodulski, A. Sukhanov, J. L. Tang, R. Teng, A. Trzupek, C. Vale, G. J. Van Nieuwenhuizen, R. Verdier, B. Wadsworth, F. L. H. Wolfs, B. Wosiek, K. Wozniak, A. H. Wuosmaa, B. Wyslouch
We present a measurement of the pseudorapidity density of primary charged particles near midrapidity in Au+Au collisions at sqrt[SNN]=130 GeV as a function of the number of participating nucleons. The pseudorapidity density, dNch/dη||η|≤1/(1/2〈Npart〉) , rises from 2.87±0.21 in peripheral events (〈Npart〉∼83) to 3.45±0.18 in central events (〈Npart〉∼ 353), which is 53±8% higher than pp̄ collisions at a similar center-of-mass energy. This is consistent with an additional contribution to charged particle production that scales with the number of binary nucleon-nucleon collisions (Ncoll).