Analyses of dNch/dη and dNch/dy distributions of BRAHMS Collaboration by means of the Ornstein-Uhlenbeck process
Interesting data on $dN_{\rm ch}/d\eta$ in Au-Au collisions ($\eta=-\ln \tan (\theta/2)$) with the centrality cuts have been reported by BRAHMS Collaboration. Using the total multiplicity $N_{\rm ch} = \int (dN_{\rm ch}/d\eta)d\eta$, we find that there are scaling phenomena among $(N_{\rm ch})^{-1}dN_{\rm ch}/d\eta = dn/d\eta$ with different centrality cuts at $\sqrt{s_{NN}} =$ 130 GeV and 200 GeV, respectively. To explain these scaling behaviors of $dn/d\eta$, we consider the stochastic approach named the Ornstein-Uhlenbeck process with two sources. The following Fokker-Planck equation is adopted for the present analyses, $$ \frac{\partial P(x,t)}{\partial t} = \gamma [\frac{\partial}{\partial x}x + \frac 12\frac{\sigma^2}{\gamma}\frac{\partial^2}{\partial x^2}] P(x, t) $$ where $x$ means the rapidity (y) or pseudo-rapidity ($\eta$). $t$, $\gamma$ and $\sigma^2$ are the evolution parameter, the frictional coefficient and the variance, respectively. Introducing a variable of $z_r = \eta/\eta_{\rm rms}$ ($\eta_{\rm rms}=\sqrt{ }$) we explain the $dn/d z_r$ distributions in the present approach. Moreover, to explain the rapidity (y) distributions from $\eta$ distributions at 200 GeV, we have derived the formula as $$ \frac{dn}{dy}=J^{-1}\frac{dn}{d \eta}, $$ where $J^{-1}=\sqrt{M(1+\sinh^2 y)}/\sqrt{1+M\sinh^2 y}$ with $M = 1 + (m/p_{\rm t})^2$. Their data of pion and all hadrons are fairly well explained by the O-U process. To compare our approach with another one, a phenomenological formula by Eskola et al. is also used in calculations of $dn/d\eta$.