Transverse Momentum and Pseudorapidity Distributions of Charged Particles and Spatial Shapes of Interacting Events in Pb-Pb Collisions at 2.76 TeV

Liu, Fu-Hu; Gao, Ya-Qin; Tian, Tian; Li, Bao-Chun

doi:https://doi.org/10.1155/2014/725739

Advances in High Energy Physics

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Volume 2014 | Article ID 725739 | https://doi.org/10.1155/2014/725739

Transverse Momentum and Pseudorapidity Distributions of Charged Particles and Spatial Shapes of Interacting Events in Pb-Pb Collisions at 2.76 TeV

Fu-Hu Liu,¹Ya-Qin Gao,¹Tian Tian,¹and Bao-Chun Li¹

Academic Editor: Bhartendu K. Singh

Received07 Feb 2014

Accepted03 Jun 2014

Published07 Jul 2014

Abstract

The transverse momentum and pseudorapidity distributions of charged particles produced in Pb-Pb collisions with different centrality intervals at center-of-mass energy per nucleon pair TeV have been analyzed by using the improved multisource thermal model in which the whole interacting system and then the sources are described by the Tsallis statistics. The modelling results are in agreement with experimental data of the ALICE Collaboration. The rapidity distributions of charged particles are obtained according to the extracted parameter values. The shapes of interacting events (the dispersion plots of charged particles) are given in the momentum, rapidity, velocity, and coordinate spaces. Meanwhile, the event shapes in different spaces consisted by different transverse quantities and longitudinal quantities are presented.

1. Introduction

Because the Relativistic Heavy Ion Collider (RHIC) run successfully in 2000, the studies of high energy heavy ion collisions have been arriving in the collider era since then. Many experiments on heavy ion collisions in GeV energy region have been finished in the past years [1–4]. The center-of-mass energy per nucleon pair () at the RHIC is superlatively 200 GeV. Presently, the most powerful heavy-ion collider in the world, the Large Hadron Collider (LHC), was built successfully in 2008-2009. Recently, the LHC does perform successful experiments on proton-proton collision at total energy of 7 TeV, proton-lead collisions at TeV, and lead-lead (Pb-Pb) collisions at TeV [5–8].

Many experiments do measure distributions and correlations of multiplicities, pseudorapidities (rapidities), transverse momentums, azimuths, and others due to that they are the “first day” measurement quantities on charged particles. Generally, these “first day” measurement quantities are studied in different centrality intervals (impacting parameters), sizes of interacting systems, center-of-mass energies, and other available dependent quantities. These charged particles are divided into positively charged particles, negatively charged particles, charged mesons, charged baryons, protons, antiprotons, and other identified charged particles according to different classifications. Even if for the transverse momentum and pseudorapidity (rapidity) distributions of charged particles, we have different interacting mechanisms and distribution regions which are considered in modelling analyses.

The transverse momentum and pseudorapidity (rapidity) distributions of charged particles contain abundant information. Studies of transverse momentum and pseudorapidity (rapidity) distributions have been persisting from fixed target experiments at accelerators to collider experiments at the RHIC and LHC. Recently, the ALICE Collaboration reported the centrality dependences of the transverse momentum and pseudorapidity distributions for charged particles in Pb-Pb collisions at TeV [8, 9]. We are interested in analyzing the ALICE data by using the current models (for a collection of many models, see [10]), particularly the multisource thermal model which was proposed by us some years ago [11–13].

In this paper, we analyze the ALICE data on transverse momentum and pseudorapidity distributions of charged particles produced in Pb-Pb collisions at TeV [8, 9] by using the improved multisource thermal model [11–13] in which the Boltzmann distribution is replaced by the Tsallis statistics [14–21]. The rapidity distributions of charged particles are obtained according to the extracted parameter values. The dispersion plots of charged particles, that is, the shapes of interacting events, are given in different spaces.

2. The Model and Method

In a given reference frame and in the rapidity space, in the framework of the multisource thermal model [11–13], many emission sources with different rapidities are assumed to form in high energy collisions. According to the values of , a target cylinder in rapidity interval , a projectile cylinder in rapidity interval , a leading target nucleon cylinder in rapidity interval , and a leading projectile nucleon cylinder in rapidity interval are assumed to form. For a symmetric collision system, we have equal relations , , , and .

In the original multisource thermal model [11–13], we have used in fact a multitemperature relativistic ideal gas model which expects a few local thermal equilibrium states existing in the collisions. Each local equilibrium state can be described by the relativistic ideal gas model (Boltzmann distribution) [22, 23] with a given temperature, and the emission of particles in the rest frame of the considered source is isotropic. This multitemperature picture can be described by the Tsallis statistics [14–21] which describes the invariant particle momentum () distribution in the rest frame of the considered source to be where is the normalization constant of the distribution, is the particle number, is the temperature parameter of the source, is a parameter (an entropic index) to characterize the degree of nonequilibrium, and , and are, respectively, the energy, rest mass, and chemical potential of the considered particle. At LHC energies, the chemical potential can be neglected due to its small value. The real free parameters in (1) are then and . Because of the introduction of the Tsallis statistics, the multisource thermal model is improved by us.

We can use the Monte Carlo method to perform the calculation based on the probability distribution of momentums where is the normalization constant. Because (2) is the probability distribution of momentums and (1) is the invariant momentum distribution, they are different in the prefactors. In the calculation, in the rest frame of the considered source with rapidity shift , various quantities such as azimuth , space angle , momentum , longitudinal momentum , and energy can be obtained. In the laboratory or center-of-mass reference frame, the rapidity , the transverse momentum , the -component of momentum , the -component of momentum , the longitudinal momentum , the energy , the space angle , and the pseudorapidity can be obtained. Meanwhile, the velocity components , , and , as well as the coordinate components , , and can be obtained, where denotes the time interval from initial collision to the stage of freeze-out. To extract more information in the calculation, we define the rapidity in -direction , the rapidity in -direction , the transverse rapidity , the transverse velocity , and the transverse coordinate .

In the following section, except for the descriptions of transverse momentum and pseudorapidity distributions and the extraction of rapidity distributions, we shall present the event shapes in momentum space , rapidity space , and velocity space (rescaled coordinate space ). Meanwhile, the event shapes in some transverse quantities [, , ()] and longitudinal quantities [, , ()] spaces are presented, too. We would like to point out that we can obtain separately rapidity and pseudorapidity distributions in the calculation. We do not need to do a conversion between the two distributions. Except for nucleus-nucleus collisions, the Tsallis statistics is also used to deal with proton-proton collision in literature [24–26].

3. Comparison and Extraction

The transverse momentum distributions of , , and produced in Pb-Pb collisions at TeV in different centrality intervals are shown in Figures 1(a)–1(c), respectively, where denotes the number of events. From up data to low one in each panel, the corresponding centrality intervals are 0–5%, 5–10%, 10–20%, , and 80–90% scaled by multiplying , and , respectively. The symbols represent the experimental data of the ALICE Collaboration [8] measured in the rapidity region and the curves are results of the Tsallis statistics. The fitted parameter values are listed in Table 1 with the values of /dof (per degree of freedom). To see clearly the dependences of parameters on centrality, the parameter values in Table 1 are also given in Figure 1(d). We can see that the temperature and nonequilibrium degree do not change in the centrality interval 0–40%. The temperature decreases and the nonequilibrium degree increases with increase of the centrality percentage in the interval 40–90%.

(a) 2.76 TeV Pb-Pb,

(b) 2.76 TeV Pb-Pb,

(c) 2.76 TeV Pb-Pb,

(d) 2.76 TeV Pb-Pb,

Figure 1

(a)–(c) Transverse momentum distributions of (a) , (b) , and (c) produced in Pb-Pb collisions at TeV in different centrality intervals 0–5%, 5–10%, 10–20%, , and 80–90% scaled by multiplying , , , , and , respectively. The symbols represent the experimental data of the ALICE Collaboration [8] and the curves are results of the Tsallis statistics. (d) Dependences of parameters and on centrality intervals. Different symbols represent the parameter values extracted from the distributions of different charged particles.

Figure 2 presents the pseudorapidity distributions of charged particles produced in Pb-Pb collisions at TeV, where denotes the number of charged particles. Figures 2(a)–2(d) correspond to the centrality intervals 0–5%, 5–10%, 10–20%, and 20–30%, respectively. The circles represent the experimental data of the ALICE Collaboration [9], and the curves are our results calculated by using the improved multisource thermal model in which the Tsallis statistics is adopted. From left to right in each panel, the dotted or dashed curves are orderly the contributions of leading target nucleons, target cylinder, projectile cylinder, and leading projectile nucleons, respectively; and the solid curve in each panel is the sum of the dotted and dashed curves. For the four panels, the parameter values obtained by fitting the experimental data are , , , , and . The other parameters GeV, , GeV, and are approximately taken from Figure 1 (Table 1), where the indexes and denote the target/projectile cylinders and the leading target/projectile nucleon cylinders, respectively. The values of /dof are 0.120, 0.141, 0.110, and 0.109, respectively.

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

In the calculation for Figure 2, only the contributions of for the target/projectile cylinders and those of for the leading target/projectile nucleon cylinders are considered due to the other contributions being small. We take as the rest mass of a charged pion (or a proton) for the target/projectile cylinders (or the leading target/projectile nucleon cylinders). Another approximation is that the parameter values obtained in (Figure 1) are used for a wide pseudorapidity range (Figure 2). The treatment for the target/projectile cylinders underestimates by ~0.01 GeV and overestimates by ~0.02. Contrarily, the second approximation overestimates and underestimates . In fact, the pseudorapidity distribution is not mainly determined by the temperature and degree of nonequilibrium but by the rapidity shifts and contribution ratio of leading nucleons. One can see that the model describes the pseudorapidity distributions of charged particles produced in Pb-Pb collisions at the LHC energy. The rapidity shifts, contribution ratio of leading nucleons, temperature, and degree of nonequilibrium do not depend obviously on the centrality percentage in the considered centrality interval 0–30%.

According to the parameter values extracted from the pseudorapidity distributions, we present the rapidity distributions of charged particles in Figure 3. For the purpose of comparison, the pseudorapidity distributions presented in Figure 2 are directly presented in Figure 3 by the dotted-dashed cures. The meanings of other curves in Figure 3 are the same as those in Figure 2. One can see the difference between the rapidity and pseudorapidity distributions of charged particles produced in Pb-Pb collisions at TeV. The differences among the four centrality intervals are not obvious except for the normalization.

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

The event shapes (dispersion plots) obtained from 1000 charged particles at the stage of freeze-out in the momentum space (or ), rapidity space (or ), and velocity space (or ) in Pb-Pb collisions in different centrality intervals at TeV are displayed in Figures 4(a)–4(d), 5(a)–5(d) and 6(a)–6(d), respectively. If we rescale coordinates , , and to , , and , respectively, Figure 6 is also the event shapes in (rescaled) coordinate space (or ). In the three figures, the closed circles, open circles, open squares, and closed squares correspond to the contributions of leading target nucleons, target cylinder, projectile cylinder, and leading projectile nucleons, respectively. One can see that the densities in the small momentum components, small () and large , small () and large , and small () and large regions are larger than those in other regions. The event shapes (dispersion plots) in the momentum, rapidity, and velocity (coordinate) spaces are obviously different. The differences in event shapes (relative density distributions in the dispersion plots) for different centrality intervals are not obvious for the considered collisions.

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

Figure 4

Extracted event shapes (dispersion plots) of 1000 charged particles at the stage of freeze-out in the momentum space (or ) in Pb-Pb collisions at TeV in the centrality intervals (a) 0–5%, (b) 5–10%, (c) 10–20%, and (d) 20–30%. The closed circles, open circles, open squares, and closed squares represent orderly the contributions of leading target nucleons, target cylinder, projectile cylinder, and leading projectile nucleons from low to high in the longitudinal rapidity space.

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

To extract more information from the pseudorapidity distributions, we present the event shapes (dispersion plots) from 1000 charged particles in Pb-Pb collisions in different centrality intervals at TeV in some spaces consisted by different transverse quantities and different longitudinal quantities. Figures 7, 8, and 9 present the results in , , and () spaces, respectively, Figures 10, 11, and 12 present the results in , , and () spaces, respectively, and Figures 13, 14, and 15 present the results in (), (), and ( or or ) spaces, respectively. The meanings of the symbols in Figures 7–15 are the same as those in Figure 4. We see different events shapes (relative density distributions in the dispersion plots) in different spaces consisted by different transverse quantities and different longitudinal quantities. The results in the same space for different centrality intervals are not obvious due to almost the same extracted parameters (except the total particle number).

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

(a) 2.76 TeV Pb-Pb, 0–5%

(b) 5–10%

(c) 10–20%

(d) 20–30%

Although we have not compared more predicted results with experimental data in the present work, the improved multisource thermal model which adopts the Tsallis statistics can describe both the transverse momentum distribution and the pseudorapidity (rapidity) distribution in high energy collisions. The transverse momentum distribution is mainly determined by the temperature and nonequilibrium degree, and the pseudorapidity distribution is mainly determined by the rapidity shifts and contribution ratio of leading nucleons.

There are some fluctuations in our calculation by using the Monte Carlo method. For example, for an event with a given centrality, different sets of random numbers render different dispersion plots, which are small statistical fluctuations from event to event. The events with different centralities correspond to large statistical fluctuations from event to event. In some case, different events may have different interacting mechanisms, which render dynamical fluctuations from event to event. The present work concerns only the statistical fluctuations.

4. Conclusions

From the above discussions, we obtain following conclusions.(a)The transverse momentum distributions of charged particles produced in Pb-Pb collisions with centrality intervals from 0–5% to 80–90% at TeV have been analyzed by using the improved multisource thermal model in which the whole interacting system and then the sources are described by the Tsallis statistics [14–21]. The modelling results are in agreement with the experimental data of the ALICE Collaboration [8]. In the centrality intervals from 0–5% to 30–40%, the temperature and nonequilibrium degree do not show a change. In the centrality intervals from 40–50% to 80–90%, the temperature decreases and the nonequilibrium degree increases with increase of the centrality percentage.(b)The pseudorapidity distributions of charged particles produced in Pb-Pb collisions with centrality intervals from 0–5% to 20–30% at TeV have been analyzed by using the improved multisource thermal model, too. The modelling results are in agreement with the experimental data of the ALICE Collaboration [9]. The contributions of the leading target nucleons, target cylinder, projectile cylinder, and leading projectile nucleons are given in different regions in the rapidity space. The rapidity shifts and contribution ratio of leading nucleons do not depend obviously on the centrality percentage in the intervals from 0–5% to 20–30%.(c)Based on the parameter values extracted from the transverse momentum and pseudorapidity distributions, the rapidity distributions of charged particles produced in Pb-Pb collisions with different centrality intervals at TeV are obtained. The contributions of the leading target nucleons, target cylinder, projectile cylinder, and leading projectile nucleons are given in different regions in the rapidity space. The rapidity shifts and contribution ratio of leading nucleons do not depend obviously on the centrality percentage in the intervals from 0–5% to 20–30%.(d)The event shapes (dispersion plots) at the stage of freeze-out in the momentum space (or ), rapidity space (or ), velocity space (or ), and coordinate space (or ) in Pb-Pb collisions in different centrality intervals at TeV are presented. The densities in the small momentum components, small () and large , small () and large , and small () and large regions are larger than those in other regions. The event shapes (dispersion plots) in the momentum, rapidity, velocity (coordinate) spaces are obviously different. The differences in event shapes (density distributions in the dispersion plots) for different centrality intervals are not obvious for the considered collisions in the considered intervals from 0–5% to 20–30%.(e)The event shapes (dispersion plots) in Pb-Pb collisions in different centrality intervals at TeV in other spaces including , , (), , , (), (), (), and ( or or ) spaces are presented. Different events shapes (density distributions in the dispersion plots) in different spaces consisted by different transverse quantities and different longitudinal quantities are obtained. The results for different centrality intervals are not obvious in the considered intervals from 0–5% to 20–30%.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work was partly finished at the State University of New York at Stony Brook, USA. One of the authors (Fu-Hu Liu) thanks Professor Dr. Roy A. Lacey and the members of the Nuclear Chemistry Group of Stony Brook University for their hospitality. The authors acknowledge the supports of the National Natural Science Foundation of China (under Grant no. 10975095, no. 11247250, and no. 11005071), the China National Fundamental Fund of Personnel Training (under Grant no. J1103210), the Open Research Subject of the Chinese Academy of Sciences Large-Scale Scientific Facility (under Grant no. 2060205), and the Shanxi Scholarship Council of China, and the Overseas Training Project for Teachers at Shanxi University.

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Copyright

Copyright © 2014 Fu-Hu Liu 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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