A Description of the Transverse Momentum Distributions of Charged Particles Produced in Heavy Ion Collisions at RHIC and LHC Energies

Hui, Jia-Qi; Jiang, Zhi-Jin; Xu, Dong-Fang

doi:https://doi.org/10.1155/2018/7682325

Advances in High Energy Physics

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Volume 2018 | Article ID 7682325 | https://doi.org/10.1155/2018/7682325

A Description of the Transverse Momentum Distributions of Charged Particles Produced in Heavy Ion Collisions at RHIC and LHC Energies

Jia-Qi Hui,¹Zhi-Jin Jiang,¹and Dong-Fang Xu¹

Academic Editor: Bhartendu K. Singh

Received05 Nov 2017

Revised27 Jan 2018

Accepted06 Mar 2018

Published08 Apr 2018

Abstract

By assuming the existence of memory effects and long-range interactions, nonextensive statistics together with relativistic hydrodynamics including phase transition are used to discuss the transverse momentum distributions of charged particles produced in heavy ion collisions. It is shown that the combined contributions from nonextensive statistics and hydrodynamics can give a good description of the experimental data in Au+Au collisions at GeV and in Pb+Pb collisions at TeV for and in the whole measured transverse momentum region and for in the region of GeV/c. This is different from our previous work using the conventional statistics plus hydrodynamics, where the describable region is only limited in GeV/c.

1. Introduction

The primary goals of the experimental programs performed in high energy heavy ion collisions are to find the deconfined nuclear matter, namely, the quark-gluon plasma (QGP), which is believed to have filled in the early universe several microseconds after the Big Bang. Therefore, studying the properties of QGP is important for both particle physics and cosmology. In the past decade, a number of bulk observables about charged particles, such as the Fourier coefficients of azimuth-angle distributions [1, 2], transverse momentum spectra [3–8], and pseudorapidity distributions [9–12], have been extensively studied in nuclear collisions at both RHIC and LHC energies. These investigations have shown that the matter created in these collisions is in the state of strongly coupled quark-gluon plasma (sQGP), exhibiting a clear collective behavior nearly like a perfect fluid with very low viscosity [13–31]. Therefore, the space-time evolution of sQGP can be described in the scope of relativistic hydrodynamics, which connects the static aspects of sQGP properties and the dynamical aspects of heavy ion collisions [32].

In our previous work [33], by considering the effects of thermalization, we once used a hydrodynamic model incorporating phase transition in analyzing the transverse momentum distributions of identified charged particles produced in heavy ion collisions. In that model, the quanta of hot and dense matter are supposed to obey the standard statistical distributions and the experimental measurements in Au+Au collisions at and 130 GeV can be well matched up in the region of GeV/c. Known from the investigations in [34, 35], the memory effects and long-range interactions might appear in the hot and dense matter. This guarantees the reasonableness of nonextensive statistics in describing the thermal motions of quanta of hot and dense matter, since this new statistics is just suitable for the thermodynamic system including memory effects and long-range interactions. Hence, in this paper, on the basis of hydrodynamics taking phase transition into consideration, we will use nonextensive statistics instead of conventional statistics to simulate the transverse collective flow of the matter created in collisions.

The nonextensive statistics are also known as Tsallis nonextensive thermostatistics, which were first proposed by Tsallis in 1988 in his pioneering work [36]. This statistical theory overcomes the shortcomings of the conventional statistics in many physical problems with long-range interactions, memory effects, or fractal space-time constrains [34]. It has a wide range of applications in high energy physics [37–39], astrophysical self-gravitating systems [40], cosmology [41], the solar neutrino problem [42], many-body theory, dynamical linear response theory, and variational methods [43].

In Section 2, a brief description is given on the employed hydrodynamics, presenting its analytical solutions. The solutions are then used in Section 3 to formulate the transverse momentum distributions of charged particles produced in heavy ion collisions in the light of nonextensive statistics and Cooper-Frye prescription. The last section is about conclusions.

2. A Brief Introduction to the Hydrodynamic Model

The key points of the hydrodynamic model [18] used in the present paper are as follows.

The expansions of fluid follow the continuity equationwhere andis the energy-momentum tensor of perfect fluid, where is the metric tensor and is the four-velocity of fluid with rapidity . The energy density and the pressure of fluid are related by the sound speed via the equation of statewhere is the temperature and is the entropy density of fluid.

Projecting (1) to the direction of giveswhich is the continuity equation for entropy conservation. Projecting (1) to the direction Lorentz perpendicular to leads to the following equation:which means the existence of scalar function satisfyingFrom and Legendre transformation, Khalatnikov potential is introduced bywhich makes the coordinates of transform towhere is the initial temperature of fluid and . In terms of , (4) can be rewritten as the so-called telegraphy equation:

With the expansions of created matter, its temperature becomes lower and lower. When the temperature reduces from initial temperature to the critical temperature , the matter transforms from the sQGP state to the hadronic state. The produced hadrons are initially in the violent and frequent collisions, which are mainly inelastic. Hence, the abundance of identified hadrons is constantly changing. Furthermore, the mean free paths of these primary hadrons are very short. In sQGP, . The evolution of them still satisfies (9) with only difference being the values of . In the hadronic state, . At the point of phase transition, is discontinuous.

The solutions of (9) for the sQGP and hadronic state are, respectively [18],where is a constant determined by fitting the theoretical results with experimental data, is the 0th-order modified Bessel function, and

3. The Transverse Momentum Distributions of Charged Particles Produced in Heavy Ion Collisions

3.1. The Energy of Quantum of Produced Matter

In the nonextensive statistics, there are two basic postulations [36, 40].

(a) The entropy of a statistical system possesses the form ofwhere is the probability of a given microstate among different ones and is a real parameter.

(b) The mean value of an observable is given bywhere is the value of an observable in the microstate .

From the above two postulations, the average occupational number of the quantum in the state with temperature can be written in a simple analytical form [44]:where is the energy of quantum and is its baryochemical potential. for fermions, and for bosons. In the limit of , it reduces to the conventional Fermi-Dirac or Bose-Einstein distributions. Hence, the value of reflects the discrepancies of nonextensive statistics from the conventional ones. Known from (15), the average energy of quantum in the state with temperature readswhere is the rapidity of quantum and is its transverse mass with rest mass and transverse momentum .

3.2. The Rapidity Distributions of Charged Particles in the State of Fluid

In terms of Khalatnikov potential , the rapidity distributions of charged particles in the state of fluid can be written as [45]whereis the area of overlap region of collisions, is impact parameter, and is the radius of colliding nucleus. From (8), the expression in the round brackets in (17) becomes

3.3. The Transverse Momentum Distributions of Charged Particles Produced in Heavy Ion Collisions

Along with the expansions of hadronic matter, its temperature becomes even lower. As the temperature drops to kinetic freeze-out temperature , the inelastic collisions among hadronic matter stop. The yields of identified hadrons remain unchanged, becoming the measured results. According to Cooper-Frye scheme [45], the invariant multiplicity distributions of charged particles take the form [18, 45, 46]where and the integrand takes values at the moment of .

Substituting in (19) by of (11), it becomeswherewhere and is the 1st-order modified Bessel function.

By using (17) and (20)–(22), we can obtain the transverse momentum distributions of identified charged particles as shown in Figures 1 and 2.

(a)

(b)

(a)

(b)

Figure 1 shows the invariant yields of , , and as a function of in Au+Au collisions at GeV. Figure 2 shows the same distributions in Pb+Pb collisions at TeV. The solid dots represent the experimental data [3, 4]. The solid curves are the results calculated from (20). It can be seen that the theoretical results are in good agreement with the experimental data for and in the whole measured region. For , the theoretical model works well in the region of GeV/c. Beyond this region, the deviation appears as shown in Figure 3, which presents the fittings for in the most peripheral collisions for up to about 4 GeV/c.

(a)

(b)

In analyses, the sound speed in hadronic state takes the value of [46–49]. The critical temperature takes the value of GeV [50]. The kinetic freeze-out temperature takes the values of 0.12 GeV for pions and kaons and 0.13 GeV for protons, respectively, from the investigations of [8], which also shows that the average value of baryochemical potential is about 0.019 GeV in Au+Au collisions. For Pb+Pb collisions, takes the value of [8]. The initial temperature in central Au+Au and Pb+Pb collisions takes the values of GeV and GeV, respectively [51].

Tables 1 and 2 list the values of , , , and /NDF in different centrality cuts. It can be seen that decreases with increasing centrality cuts. The value of , affecting the slopes of curves, is slightly larger than 1 for different kinds of charged particles. It is almost irrelevant to centrality cuts, while it increases with increasing beam energies and the masses of charged particles.

The parameter has the same effects as on curves. They all affect the heights of the curves. The fitted in Tables 1 and 2 gives the ratiosThese ratios are in good agreement with the relative abundance of particles and antiparticles given in [3, 4]. This agreement may be due to the fact that the integrand of (20) is the same for particles and antiparticles in case that takes a common constant for these two kinds of particles. Hence, might be proportional to the abundance of corresponding particles.

4. Conclusions

By introducing the nonextensive statistics, we employ the relativistic hydrodynamics including phase transition to discuss the transverse momentum distributions of charged particles produced in heavy ion collisions. The model contains rich information about the transport coefficients of fluid, such as the initial temperature , the critical temperature , the kinetic freeze-out temperature , the baryochemical potential , the sound speed in sQGP state , and the sound speed in hadronic state . Except for , the other five parameters take the values either from widely accepted theoretical results or from experimental measurements. As for , there are no widely acknowledged values so far. In this paper, takes the values referring to other studies for the most central collisions, and, for the rest of centrality cuts, is determined by tuning the theoretical results to experimental data. The present investigations show the conclusions as follows:

The theoretical model can give a good description of the experimental data in Au+Au collisions at GeV and in Pb+Pb collisions at TeV for and in the whole measured transverse momentum region and for in the region of GeV/c.

The fitted is close to 1. This might mean that the difference between nonextensive statistics and conventional statistics is small. However, it is this small difference that plays an essential role in extending the fitting region of .

The fitted increases with beam energies and the masses of charged particles. This might mean that the nonextensive statistics are more suitable for these conditions.

The model cannot describe the experimental measurements for in the region of GeV/c for the both kinds of collisions. This might be caused by the hard scattering process [52]. To improve the fitting conditions, the results from perturbative QCD should be taken into account.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

This work is supported by the Shanghai Key Lab of Modern Optical System.

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Copyright © 2018 Jia-Qi Hui et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The publication of this article was funded by SCOAP³.

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