2011Physical Review COpen access

Charged-particle multiplicity and pseudorapidity distributions measured with the PHOBOS detector in Au+Au , Cu+Cu , d+Au , and p+p collisions at ultrarelativistic energies

B. Alver, B. B. Back, M. D. Baker, M. Ballintijn, D. S. Barton, R. R. Betts, A. A. Bickley, R. Bindel, A. Budzanowski, W. Busza, A. Carroll, Z. Chai, V. Chetluru, M. P. Decowski, E. Garcı́a, T. Gburek, N. George, K. Gulbrandsen, S. Gushue, C. Halliwell, J. Hamblen, G. A. Heintzelman, C. Henderson, D. J. Hofman, R. S. Hollis, R. Hołyński, B. Holzman, A. Iordanova, E. Johnson, J. L. Kane, J. Katzy, N. Khan, J. Kotuła, W. Kucewicz, P. Kulinich, C. M. Kuo, W. Li, W.T. Lin, C. Loizides, S. Manly, D. McLeod, J. Michałowski, A. C. Mignerey, R. Nouicer, A. Olszewski, R. Pak, I. C. Park, H. Pernegger, Catherine L. Reed, L. P. Remsberg, M. Reuter, C. Roland, G. Roland, L. J. Rosenberg, J. Sagerer, Pankaj Sarin, P. Sawicki, I. Sedykh, W. Skulski, Christopher Smith, S. G. Steadman, P. Steinberg, G. S. F. Stephans, M. Stodulski, A. Sukhanov, M. B. Tonjes, A. Trzupek, C. Vale, G. J. van Nieuwenhuizen, S. S. Vaurynovich, R. Verdier, G. I. Veres, B. Wadsworth, Peter Walters, E. A. Wenger, F. L. H. Wolfs, B. K. Wosiek, K. W. Woźniak, A. H. Wuosmaa, B. Wysłouch

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Abstract

Pseudorapidity distributions of charged particles emitted in $\text{Au}+\text{Au}$, $\text{Cu}+\text{Cu}$, $d+\text{Au}$, and $p+p$ collisions over a wide energy range have been measured using the PHOBOS detector at the BNL Relativistic Heavy-Ion Collider (RHIC). The centrality dependence of both the charged particle distributions and the multiplicity at midrapidity were measured. Pseudorapidity distributions of charged particles emitted with $|\ensuremath{\eta}|<5.4$, which account for between 95% and 99% of the total charged-particle emission associated with collision participants, are presented for different collision centralities. Both the midrapidity density ${\mathit{dN}}_{\text{ch}}/d\ensuremath{\eta}$ and the total charged-particle multiplicity ${N}_{\text{ch}}$ are found to factorize into a product of independent functions of collision energy, $\sqrt{{s}_{{}_{\mathit{NN}}}}$, and centrality given in terms of the number of nucleons participating in the collision, ${N}_{\text{part}}$. The total charged particle multiplicity, observed in these experiments and those at lower energies, assumes a linear dependence of $(\mathrm{ln}{s}_{{}_{\mathit{NN}}}){}^{2}$ over the full range of collision energy of $\sqrt{{s}_{{}_{\mathit{NN}}}}=2.7$--200 GeV.

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Pseudorapidity distributions of charged particles emitted in $\text{Au}+\text{Au}$, $\text{Cu}+\text{Cu}$, $d+\text{Au}$, and $p+p$ collisions over a wide energy range have been measured using the PHOBOS detector at the BNL Relativistic Heavy-Ion Collider (RHIC). The centrality dependence of both the charged particle distributions and the multiplicity at midrapidity were measured. Pseudorapidity distributions of charged particles emitted with $|\ensuremath{\eta}|<5.4$, which account for between 95% and 99% of the total charged-particle emission associated with collision participants, are presented for different collision centralities. Both the midrapidity density ${\mathit{dN}}_{\text{ch}}/d\ensuremath{\eta}$ and the total charged-particle multiplicity ${N}_{\text{ch}}$ are found to factorize into a product of independent functions of collision energy, $\sqrt{{s}_{{}_{\mathit{NN}}}}$, and centrality given in terms of the number of nucleons participating in the collision, ${N}_{\text{part}}$. The total charged particle multiplicity, observed in these experiments and those at lower energies, assumes a linear dependence of $(\mathrm{ln}{s}_{{}_{\mathit{NN}}}){}^{2}$ over the full range of collision energy of $\sqrt{{s}_{{}_{\mathit{NN}}}}=2.7$--200 GeV.

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Available abstract

Pseudorapidity distributions of charged particles emitted in $\text{Au}+\text{Au}$, $\text{Cu}+\text{Cu}$, $d+\text{Au}$, and $p+p$ collisions over a wide energy range have been measured using the PHOBOS detector at the BNL Relativistic Heavy-Ion Collider (RHIC). The centrality dependence of both the charged particle distributions and the multiplicity at midrapidity were measured. Pseudorapidity distributions of charged particles emitted with $|\ensuremath{\eta}|<5.4$, which account for between 95% and 99% of the total charged-particle emission associated with collision participants, are presented for different collision centralities. Both the midrapidity density ${\mathit{dN}}_{\text{ch}}/d\ensuremath{\eta}$ and the total charged-particle multiplicity ${N}_{\text{ch}}$ are found to factorize into a product of independent functions of collision energy, $\sqrt{{s}_{{}_{\mathit{NN}}}}$, and centrality given in terms of the number of nucleons participating in the collision, ${N}_{\text{part}}$. The total charged particle multiplicity, observed in these experiments and those at lower energies, assumes a linear dependence of $(\mathrm{ln}{s}_{{}_{\mathit{NN}}}){}^{2}$ over the full range of collision energy of $\sqrt{{s}_{{}_{\mathit{NN}}}}=2.7$--200 GeV.

Key concepts: Pseudorapidity, Physics, Multiplicity (mathematics), Charged particle, Nuclear physics, Range (aeronautics), Collision, Particle physics

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Charged-particle multiplicity and pseudorapidity distributions measured with the PHOBOS detector in Au+Au , Cu+Cu , d+Au , and p+p collisions at ultrarelativistic energies — Research Paper | ScholarLens