标题： BRAHMS合作组通过奥尔施泰因-乌伦贝克过程对$dN_{ch}/dη$和$dN_{ch}/dy$分布的分析 显示英文标题

标题： Analyses of $dN_{ch}/dη$ and $dN_{ch}/dy$ distributions of BRAHMS Collaboration by means of the Ornstein-Uhlenbeck process

摘要： 关于Au-Au碰撞（$\eta=-\ln \tan (\theta/2)$）中$dN_{\rm ch}/d\eta$的有趣数据已由BRAHMS合作组报告。 利用总多重性$N_{\rm ch} = \int (dN_{\rm ch}/d\eta)d\eta$，我们发现不同中心度切割下$(N_{\rm ch})^{-1}dN_{\rm ch}/d\eta = dn/d\eta$在$\sqrt{s_{NN}} =$130 GeV和200 GeV时存在标度现象。 为了解释$dn/d\eta$的这些标度行为，我们考虑了一种名为具有两个源的Ornstein-Uhlenbeck过程的随机方法。 以下采用福克-普朗克方程进行当前分析，$$ \frac{\partial P(x,t)}{\partial t} = \gamma [\frac{\partial}{\partial x}x + \frac 12\frac{\sigma^2}{\gamma}\frac{\partial^2}{\partial x^2}] P(x, t) $$其中$x$表示快度(y)或伪快度($\eta$)。$t$，$\gamma$和$\sigma^2$分别是演化参数、摩擦系数和方差。 引入变量$z_r = \eta/\eta_{\rm rms}$ ($\eta_{\rm rms}=\sqrt{< \eta^2 >}$) 我们在目前的方法中解释了$dn/d z_r$分布。此外，为了从 200 GeV 的$\eta$分布解释快度 (y) 分布，我们推导了公式$$ \frac{dn}{dy}=J^{-1}\frac{dn}{d \eta}, $$其中$J^{-1}=\sqrt{M(1+\sinh^2 y)}/\sqrt{1+M\sinh^2 y}$与$M = 1 + (m/p_{\rm t})^2$。它们的介子和所有强子的数据由 O-U 过程很好地解释。为了将我们的方法与其他方法进行比较，提出了 Eskola 等人的经验公式。 也用于$dn/d\eta$的计算中。 显示英文摘要

摘要： 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 $z_r = \eta/\eta_{\rm rms}$ ($\eta_{\rm rms}=\sqrt{< \eta^2 >}$) 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 $dn/d\eta$.