Abstract. Charged particle pseudorapidity densities are presented for the 197Au + 197Au reaction at√sNN = 130 GeV. These densities provide an essential characteriza-tion of the underlying reactions mechanisms for ultra-relativistic heavy-ion collisions. This talk details how the global charged particle yields are measured at BRAHMS and presents some preliminary results from the analysis of data taken during the first year of the RHIC experimental program
Pseudorapidity density and multiplicity distributions of charged particles produced in heavy-ion col...
The charged particles produced in nucleus-nucleus collisions are divided into two parts. One is from...
Abstract The BRAHMS experiment at RHIC has measured the rapidity distribution of charged pions, kaon...
We present the results obtained by the BRAHMS experiment at the Relativistic Heavy Ion Collider (RHI...
Charged-particle pseudorapidity densities are presented for the d+Au reaction at sqrt{s_{NN}}=200 Ge...
We present charged-particle multiplicities as a function of pseudorapidity and collision centrality ...
We present the first measurements of the pseudorapidity distribution of primary charged particles in...
In heavy ion collisions, charged particles come from two parts: the hot and dense matter and the lea...
Au+Au collisions in the Relativistic Heavy Ion Collider (RHIC) herald a new era of opportunities for...
The charged-particle pseudorapidity density for Au+Au collisions at sqrt(s_NN)=62.4 GeV has been mea...
Multiplicity and pseudorapidity (η) density (dNch/dη) distributions of charged hadrons provide key i...
We present measurements of the pseudorapidity distribution of primary charged particles produced in ...
We present measurements of the pseudorapidity (η ) distribution of charged particles (dN<SUB>ch</SUB...
Pseudorapidity distributions of charged particles emitted in Au+Au, Cu+Cu, d+Au, and p+p collisions ...
The charged-particle pseudorapidity density measured over four units of pseudorapidity in nonsingle-...
Pseudorapidity density and multiplicity distributions of charged particles produced in heavy-ion col...
The charged particles produced in nucleus-nucleus collisions are divided into two parts. One is from...
Abstract The BRAHMS experiment at RHIC has measured the rapidity distribution of charged pions, kaon...
We present the results obtained by the BRAHMS experiment at the Relativistic Heavy Ion Collider (RHI...
Charged-particle pseudorapidity densities are presented for the d+Au reaction at sqrt{s_{NN}}=200 Ge...
We present charged-particle multiplicities as a function of pseudorapidity and collision centrality ...
We present the first measurements of the pseudorapidity distribution of primary charged particles in...
In heavy ion collisions, charged particles come from two parts: the hot and dense matter and the lea...
Au+Au collisions in the Relativistic Heavy Ion Collider (RHIC) herald a new era of opportunities for...
The charged-particle pseudorapidity density for Au+Au collisions at sqrt(s_NN)=62.4 GeV has been mea...
Multiplicity and pseudorapidity (η) density (dNch/dη) distributions of charged hadrons provide key i...
We present measurements of the pseudorapidity distribution of primary charged particles produced in ...
We present measurements of the pseudorapidity (η ) distribution of charged particles (dN<SUB>ch</SUB...
Pseudorapidity distributions of charged particles emitted in Au+Au, Cu+Cu, d+Au, and p+p collisions ...
The charged-particle pseudorapidity density measured over four units of pseudorapidity in nonsingle-...
Pseudorapidity density and multiplicity distributions of charged particles produced in heavy-ion col...
The charged particles produced in nucleus-nucleus collisions are divided into two parts. One is from...
Abstract The BRAHMS experiment at RHIC has measured the rapidity distribution of charged pions, kaon...