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Joint Institute for Nuclear Research Relativistic ... - Index of - JINR

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NET CHARGE FLUCTUATIONS IN AA COLLISIONS IN A SIMPLE<br />

STRING-INSPIRED MODEL<br />

A.V. Titov 1† , V.V. Vechernin 1<br />

(1) Saint Petersburg State University<br />

† E-mail: arsenii.titov@gmail.com<br />

Net charge fluctuations have been proposed as a possible indicator <strong>of</strong> the <strong>for</strong>mation<br />

<strong>of</strong> quark-gluon plasma in high-energy nucleus-nucleus collisions [1, 2]. The theoretical<br />

predictions <strong>of</strong> the value <strong>of</strong> the fluctuations [1, 2, 3] do not directly consist with the experimental<br />

results from RHIC [4]. At present the results extracted from ALICE experimental<br />

data have also rather ambiguous interpretation in the framework <strong>of</strong> existing models [5].<br />

In this connection, we try to describe the experimental data in the framework <strong>of</strong> an<br />

alternative string-inspired model.<br />

We introduce two effective sources <strong>of</strong> thehadron production. The first source emulates<br />

the mid-rapidity particle production from the decays <strong>of</strong> the strings. In the string model<br />

one has an approximate conservation <strong>of</strong> the charge locally in rapidity, so we assume this<br />

source emits N 1+ positive and N 1− negative particles in the central rapidity interval ∆y<br />

with the same mean values and variances, but due to “leakage” <strong>of</strong> the charge on the<br />

borders <strong>of</strong> the interval N 1+ ≠ N 1− event-by-event. In string models the positive charge<br />

<strong>of</strong> initial nuclear protons is associated with their valence quarks and is concentrated at<br />

projectile and target rapidities. The transport <strong>of</strong> this charge into the mid-rapidity region<br />

∆y is the second cause <strong>of</strong> the deviation <strong>of</strong> the charge from zero in this region. To simulate<br />

this process we introduce the second source which produces only positive particles.<br />

As a result the measure <strong>of</strong> the dynamical net charge fluctuations, ν dyn , is expressed in<br />

terms <strong>of</strong> the model parameters. The parameters <strong>of</strong> the first (main) source are expressed<br />

through the parameters characterizing the individual string and their event-by-event distribution.<br />

The important feature <strong>of</strong> the model is that based on the results obtained in [6]<br />

we do not assume that the engaged fluctuations are poissonian.<br />

The model calculations are compared with the experimental data on pseudorapidity<br />

dependence <strong>of</strong> ν dyn from RHIC [4]. It is shown that under some assumptions the obtained<br />

results are consistent with the data.<br />

References<br />

[1] S. Jeon and V. Koch, Phys. Rev. Lett. 85, 2076 (2000).<br />

[2] M. Asakawa, U. Heinz and B. Muller, Phys. Rev. Lett. 85, 2072 (2000).<br />

[3] E.V. Shuryak and M.A. Stephanov, Phys. Rev. C 63, 064903 (2001).<br />

[4] B.I. Abelev et al. (STAR Collaboration), Phys. Rev. C 79, 024906 (2009).<br />

[5] S. Jena <strong>for</strong> the ALICE Collaboration, arXiv:1203.0542 [nucl-ex] (2012).<br />

[6] V.V. Vechernin and H.S. Nguyen, Phys. Rev. C 84, 054909 (2011).<br />

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