Advances in High Energy Physics

Volume 2013, Article ID 908046, 7 pages

http://dx.doi.org/10.1155/2013/908046

## Transverse Momentum, Centrality, and Participant Nucleon Number Dependence of Elliptic Flow

^{1}Department of Physics, Shanxi University, Taiyuan, Shanxi 030006, China^{2}Department of Mathematics, Business College of Shanxi University, Taiyuan, Shanxi 030031, China

Received 25 July 2012; Revised 9 November 2012; Accepted 12 November 2012

Academic Editor: John W. Norbury

Copyright © 2013 Bao-Chun Li 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.

#### Abstract

In the combined framework of a multisource and participant-spectator model, we study the elliptic flow as a function of transverse momentum and number of participating nucleons in GeV Au-Au and TeV Pb-Pb collisions and argue that the geometry of the initial overlap region in the collisions determines the experimentally measured azimuthal asymmetries. Our results are approximately in agreement with the data from PHENIX and ALICE collaborations.

#### 1. Introduction

Elliptic flow is one of the key observables to study the properties of the Quark-Gluon plasma (QGP) created at the early stage of high-energy collisions and is generated in a collective expansion of the hot and dense matter. In years of experiments at the relativistic heavy ion collider (RHIC), one of the most important discoveries is the large elliptic flow in noncentral nucleus-nucleus collisions, which is a clear indication of a collective behavior. As a signature of a collective flow in relativistic nuclear collisions, the elliptic flow was also observed at the AGS and SPS. In a thermodynamical picture, the asymmetric distribution of the initial energy density causes a larger pressure gradient in the shortest direction of the ellipsoidal medium, which can turn the spatial anisotropy of the produced hot matter into a flow anisotropy in the momentum distributions of measurable final-state particles [1, 2]. Therefore, the main interest in the elliptic flow study grew from its sensitivity to the system properties at very early stage in the system evolution.

Elliptic flow is an informative quantity in better understanding the properties of the hot dense matter created during the initial stage of high-energy collisions. Additionally, the study of the elliptic flow dependence on collision geometry provides insight into the degree of thermalization, transport coefficients, and the equation of state (EOS) of the produced medium [3, 4]. In order to fit the elliptic flow, the hydrodynamic simulation shows that a very small shear viscosity is required [5, 6]. It is believed that a strongly coupled QGP (sQGP) created at RHIC behaves like a nearly perfect fluid [7]. The ideal hydrodynamics has been successful in explaining the observed collective flow at low transverse momentum [5, 6]. Moreover, many collaborations, such as the STAR Collaboration [8], the PHENIX Collaboration [9], and ALICE Collaboration [10], are involved in this field. For theoretical description or experimental analysis, one can easily find elliptic flows as a function of transverse momentum [9–11], rapidity or pseudorapidity [12, 13], centrality percent or impact parameter [14, 15], transverse kinetic energy [11], normalized particle multiplicity [14], and so forth.

The elliptic flow is quantified by the second harmonic Fourier coefficient of the azimuthal angle distribution of final-state particles with respect to the reaction plane; that is, where is the azimuthal angle, is the event plane angle, and angular brackets denote a statistical average over many particles and events. In our previous work [16], we have investigated the transverse momentum dependence of elliptic flow in Au-Au collisions at the RHIC energy and in Pb-Pb collisions at the LHC energy. In this work, we focus our attention on the dependence of elliptic flows on both transverse momentum and number of participants, which is directly related to the centrality and eccentricities in the Glauber model. The elliptic flow dependence on the geometry of collisions is of particular importance, as the flow is thought to depend heavily on the initial spatial anisotropy. Therefore, the basic idea of our model is that the angular azimuthal anisotropy is associated with the geometry of the first stages in the collision, where the projected overlap region is in the shape of an almond with the long axis perpendicular to the interaction plane. This paper is organized as follows. In Section 2, we introduce the model and formulation that builds a connection between the multi-source model [17, 18] and the participant-spectator model [19]. In Section 3, we present our results, which are compared with the experimental data. The discussion and the summary are given in Sections 4 and 5.

#### 2. Elliptic Flow and Number of Participant Nucleons

In order to understand the elliptic flow dependence on transverse momentum and number of participating nucleons, we use the multi-source model [17, 18] and a geometrical picture of the participant-spectator model [19] in this work. By fitting data, we may find the connection between the two models.

First, we simply describe the multi-source model. At the initial stage of nucleus-nucleus collisions, numerous primary nucleon-nucleon collisions occur. The primary nucleon-nucleon collision can be regarded as an emission source at intermediate energy or a few sources at high energy. The participant nucleons in primary collisions have probabilities to take part in cascade collisions. Meanwhile, the particles produced in primary or cascade nucleon-nucleon collisions have probabilities to take part in secondary collisions with the latter nucleons and other particles. Each cascade (or secondary) collision is also regarded as an emission source or a few sources. Many such emission sources of final-state particles are expected to be formed in the collision process, and each source is considered to emit particles isotropically in the rest frame of the source. There are interactions among the emission sources due to the mechanics and electromagnetism effects. The interactions will cause the source to depart from the isotropic emission. In order to describe the anisotropic source, the source deformation and movement have been introduced in the model [17, 18, 21]. In the rest frame of the source, the three momentum components , , and of the considered particle have Gaussian distributions with the same standard deviation . The distributions of the momentum components and are

Considering the interaction with other emission sources, the source will have deformations and movements along the and axis; the momentum components will be modified to where and represent the deformation and movement of the emission source, respectively. Generally speaking, different or can be obtained for events with different centralities (or impact parameters). In the ultrarelativistic nuclei collision at the nonzero impact parameter the overlap area in the transverse plane has a short axis () which is parallel to the impact parameter and a long axis which is perpendicular to the impact parameter. Anisotropy in the central region of collisions is driven by the almond shape of the overlapping area [3, 22, 23], which is converted by the pressure gradient into a momentum asymmetry. More particles are emitted along and the anisotropy intensity is denoted by the coefficient , which is directly sensitive to the change in the initial spatial geometry. As the overlap expands, the system becomes more spherical, and the driving force quenches itself gradually. With the increase of or of the particles produced in the collisions, the momentum anisotropy decreases. Therefore, for the concerned centrality, is not a constant but a function of the momentum. We set empirically the function where the expansion factor indicates the magnitude of the expansion and and denote the contributions of and , respectively. With (3), the joint probability density function of transverse momentum and azimuthal angle is Then, the elliptic flow is given by where is the azimuthal angle of the particle, angular brackets denote a statistical average over many particles and events, and is an event plane angle and defined as For convenience, we can also compute the transverse momentum and elliptic flow by using the Monte Carlo calculation:where , , , and denote random numbers in .

The incoming direction of the projectile nucleus is along the axis, and the reaction plane is defined as the plane. The minimum distance between the centers of the target and projectile nuclei in collisions is denoted to be the impact parameter . In the fireball participant-spectator model [19], the final particles are emitted from a composite system formed by the overlap between the projectile and target nuclei. According to the participant-spectator model in nucleus-nucleus collisions, the participant is the overlapping region of the two nuclei, and the spectator is the other part outside the overlapping region. Using the geometrical concepts of the participant-spectator model, the nucleon numbers in the target and projectile participants are given by respectively, where and are the projectile and target radius. The nuclear density function for an even distribution is , and for a heavy nucleus with mass number greater than 16, there is a two-parameter Fermi distribution [24]. Then, we have respectively, where , (), and represent the normalized constant, nuclear radius, and skin depth, respectively. The parameters are taken as fm and fm, for Au + Au, and fm, and fm, for Pb + Pb, based on data from low energy electron-nucleus scattering experiments [25]. Although the nuclear densities of Au and Pb nuclei are the experimental charge densities, the difference in the neutron densities has little effect on the number of participant nucleons. The total nucleon numbers in the two participants are

As can be clearly seen from the above discussion, the correlation between and calculated by the geometrical structure named the participant-spectator model has been given. is a well-understood quantity that is directly related to the centrality and calculated eccentricities in the Glauber model. However, we also want to know the relationship between the elliptic flow and the number of participants. So, it is naturally that the multi-source model was introduced from previous works.

#### 3. Comparison with Experimental Data

In Figure 1, we show elliptic flows as a function of transverse momentum for charged hadrons produced in = 200 GeV Au-Au collisions and = 2.76 TeV Pb-Pb collisions. The symbols represent the experimental data of the PHENIX Collaboration [20] and the ALICE Collaboration [10]. The curves are our computed results with different , which are determined by fitting the data and are given as a function of centrality percent in Figure 2(a). The other parameters used for the calculations are and (Figure 1(a)) and and (Figure 1(b)), which are determined by fitting the data and the increase with center of energy and are independent of centralities. It is obvious that increases with in the low region, as predicted by ideal hydrodynamic calculations. The observed saturates or decreases in the region of GeV/. However, ideal hydrodynamic model calculations show that increases with in this region [4]. One can see that the calculated results are in agreement with the experimental data in the whole observed region for all concerned centralities.

The square values of the expansion factor used for Figure 1 are displayed in Figure 2(a), by different symbols as marked. Obviously, tends to a saturation for the more peripheral collisions (>50%). We find that, except for the saturation region, the values of are approximately proportional to the centrality percent . By the geometric relation of the to the impact parameter [27], we have which holds to a very high accuracy for all but most peripheral collisions, and represents the nuclear radius of Au(Pb). Then, the dependence of the expansion factor on the is obtained and displayed in Figure 2(b). increases linearly with increasing the impact parameter from the most central (0–10%) to the mid-peripheral (40–50%) collisions. From Figure 1, we notice that tends to saturation for the more peripheral collisions (>50%) in = 200 GeV Au-Au collisions and = 2.76 TeV Pb-Pb collisions. So, it renders that has a saturation at large . As shown in Figure 2(b), the saturation happens at fm. Except for the saturation region, the values of exhibit a linear dependence on the impact parameter . This linear dependence corresponds to a range from the most central (0–10%) to the mid-peripheral (40–50%) collisions. For Au-Au and Pb-Pb collisions, in the linear (or non-saturation) region, we obtain and , respectively. The slope for Pb-Pb collisions increases by about over Au-Au collisions.

In heavy-ion collisions, initial geometric quantities such as the impact parameter and the shape of the collision region cannot be directly determined experimentally. However, it is possible to relate the elliptic flow and number of observed particles to the centrality of the collisions. Using the percentile centrality of a collision, the initial geometric configuration can be estimated with models [23, 27–30]. In terms of elliptic flows, the almond shaped interaction volume produced in a noncentral collision is converted by the pressure gradient into a momentum asymmetry. For final particles, the interaction of the emission sources is related to the hot dense matter in sources and also results in the azimuthally anisotropic expansion in the momentum space [31].

With fitting the data of , the parameters used for the calculations are obtained. And then, combining the above linear relation between and with (12), we can compute the elliptic flows as a function of the participant nucleon number in = 200 GeV Au-Au collisions and = 2.76 TeV Pb-Pb collisions, which are shown in Figures 3(a) and 3(b), respectively. The symbols represent the experimental data of the PHENIX Collaboration [20] and the ALICE Collaboration [26]. It is obvious that decreases with the increase of . One can see that except for the very peripheral collisions (very low ), the calculated results are approximately in agreement with the experimental data of for different transverse momentum ranges.

#### 4. Discussion of the Results

We have presented the results of azimuthal anisotropy using the elliptic flow as a function of and in GeV Au-Au collisions and = 2.76 TeV Pb-Pb collisions. Elliptic flow dependence on is well described for a wide range of transverse momentum values in the framework of the multi-source model. The parameter in the model is used to reflect the expansion of momenta. An isotropic emission corresponds to the expansion factor . Significantly, the detailed comparison between the calculation results and the experimental data proved that increases linearly with the impact parameter from the most central (0–10%) to mid-peripheral (40–50%) collisions. The behavior is due to the change in initial eccentricity of the initial fireball from central to peripheral events at each centrality [32, 33]. In the combined analysis of the multi-source model and the participant-spectator model, the double differential flow coefficients can be obtained. It is found that except for the very peripheral collisions, the results are approximately in agreement with the experimental data from the PHENIX and ALICE Collaborations.

Our treatment of correlation is very simple. According to the participant-spectator model [23], the participant nucleon number at a given impact parameter can be calculated by a geometrical picture. is a well-understood quantity that is directly related to the centrality and the calculated eccentricities in the Glauber model. The expansion coefficient in the multi-source model [17, 18] is related to (or centrality percent ) by fitting the data of , where a linear relationship between and is obtained by using a realistic description of the nuclear geometry in a Glauber calculation [24]. In this case, a connection between and via has been built in the combined framework of the two models. Such geometric calculations will be helpful to understand the baseline physics of heavy ions at the LHC in terms of nuclear geometry. Future heavy ion experiments, both at the RHIC and the LHC, will further push our understanding of nuclear geometry.

The elliptic flow originates from the spatial anisotropy of the initial overlap volume in noncentral nucleus-nucleus collisions. It is one of the most informative quantities in better understanding the nature and properties of the matter in high-energy nuclear collisions. The ideal hydrodynamic model calculations reproduce the mass ordering of in the relatively low region but overshoot the values of for all centrality bins [34]. To understand the viscous nature of QGP, the dissipative hydrodynamics have recently been applied to explain the experimental data of by including the effect of shear and bulk viscosity [35–37]. The study of the elliptic flow in our simple model, where the system expansion can be quantified in the momentum space, shows that the expansion factor is expressed by the impact parameter , which is related to the number of participants using a realistic description of the nuclear geometry in a Glauber calculation [24].

#### 5. Summary and Conclusions

Summarizing up, using the combined framework of the multi-source model [17, 18] and the participant-spectator model [19], we have investigated the elliptic flow of final-state particles produced in nucleus-nucleus collisions.The model is able to describe the dependence of the elliptical flow on transverse momentum and number of participants (or centrality). The model is too simplistic to give the geometrical picture of nucleus-nucleus collisions. However, it proves to be helpful to understand the anisotropic momentum distribution and (or centrality) dependence of various elliptic flows. Particularly, this model is successful in the descriptions of (pseudo) rapidity and multiplicity distributions for produced particles [17, 18]. In the description of , the present work is a successful attempt.

#### Acknowledgments

This work is supported by the National Natural Science Foundation of China under Grant no. 11247250, no. 10975095 and no. 11005071, the National Fundamental Fund of Personnel Training (J1103210), the Shanxi Provincial Natural Science Foundation under Grant no. 2011011001, and the Open Research Subject of the Chinese Academy of Sciences-Large-Scale Scientific Facility (2060205).

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