Abstract
We study the effects of empty sites in the prisoner’s dilemma game based on social diversity by introducing some empty sites into a square lattice. The results reveal that the empty sites dramatically enhance the cooperation level for a wide range of temptation to defection values if two types of players coexist. By calculating the chances of different type-combinations of the players located on the square lattice, we find that there is an intermediate region where five social ranks are induced to satisfy the certain rank distributions and the cooperation level is significantly enhanced. Moreover, simulation results also show that the moderate gaps among the social ranks can favor cooperation for a larger occupation density.
1. Introduction
Cooperation is fundamental to biological and social systems. Thus, it is a crucial issue to find and understand what kinds of factors facilitate cooperation. Over the past decades, various versions of evolutionary games have been studied extensively to explore the possibilities for enhancing the cooperative behavior among selfish individuals. Consequently, different mechanisms, for example, kin selection [1], direct [2] and indirect [3] reciprocity, spatial reciprocity [4], voluntary participation [5], and chaotic variations to the payoffs [6], are found to urge the emergence of cooperative behavior in biological systems as well as within human societies [7]. Among all the above mechanisms, the spatial reciprocity has not become an active and important topic until Nowak and May [8] introduced their seminal theoretical mechanism about game and spatial chaos. In recent years, topological inhomogeneities have been introduced to promote the level of cooperation [9–13]. Some investigations suggested that complex networks were beneficial for the evolution of cooperation if its connectivity structure was similar to that of social networks [14–18]. Besides the topological inhomogeneities, inhomogeneities of individual personality have also been introduced [19, 20], because of the fact that inhomogeneities of individual personality are the common features of society. Several authors have reported that some distinguished players have the stronger capacities to spread their own strategies, resulting in the thriving of cooperation when the system consists of two types of players with asymmetric teaching and learning activities [21–27]. For example, Droz et al. [21] suggested that the cooperation could be greatly enhanced if there was a relevant difference of the strategy transfer capability between the influential players and their followers. Szolnoki and Szabó [22] found that cooperation could be supported for those models where a portion of players had stronger activities in spreading their own strategies than their neighbors. Li et al. [23] modified the classical spatial game [8] by dividing the population into different types and found that cooperation was significantly promoted for a wide range of the temptation to defection parameters. The study of disordered environments or diluted lattices is another important method in spatial games. Apart from the previous investigation presented by Vainstein and Arenzon [28], there are many reports about the effects of population density on cooperation in recent years [29–32]. For example, Wang et al. [29, 30] found that the percolation threshold of an interaction graph constituted the optimal population density for the evolution of cooperation. Mitteldorf and Wilson [31] found that patches of cooperators were more favorable at the high density than patches of defectors if the population density was permitted to fluctuate. Nowak et al. [32] investigated interaction between the individuals inside a region of radius on a diluted square lattice and found that the polymorphism of cooperators and defectors was persistent if was not too large.
Despite that several authors [33–35] have reviewed the progress of spatial evolutionary games recently, few reports are related to the elucidation of the effect of population density on cooperation in inhomogeneous society. There are still scarce data about the combined effects of both inhomogeneities and population density on cooperation and further efforts are eagerly required. In order to explore how cooperation is influenced by population density in inhomogeneous society, we study the evolution of cooperation in the prisoner’s dilemma game on a square lattice with the periodic boundary conditions. In this model, the empty sites, A players, and B players are randomly located on the sites of the square lattice with different concentrations, respectively.
In this paper, we preliminarily focus on spatial game. Further, we only consider how the population density and the social diversity affect the cooperation between individuals. The paper is organized as follows. At first, the details of the model are presented and the parameters of the model are defined in Section 2. Subsequently, the main simulation results and discussions will be presented in Section 3. Finally, the conclusion is summarized in the last section.
2. Model
We consider an evolutionary prisoner’s dilemma game on a square lattice with the periodic boundary conditions, where two types of players (A and B) are located on the sites of a square lattice with the different concentrations, respectively. Different from the original version of the prisoner’s dilemma based on social diversity [23], we assume that some sites are empty. To describe the occupation of the site (), we take to be either 1, if the site is occupied, or 0, otherwise. We define the density of players , where is the number of cooperators and is the number of defectors. Initially, the empty sites and two types of players (A and B) are distributed randomly and a player is designated as a cooperator or defector with the equal percentage. We define the density of A players, , where is the number of A players. In this model, we only consider the simplest case of pure strategies, cooperation (C) and defection (D), represented by the variable and 0, respectively. The neighborhood is restricted to the nearest neighbors of site and self-interactions are excluded.
Each Monte Carlo (MC) simulation procedure has two elementary steps. Firstly, all individuals play the game against all their four nearest neighbors (if present) and collect the payoffs from the combats according to the parameterized payoff matrix suggested by Li et al. [23]. That is to say, when two neighboring players play the game, if they are of the same type (namely, both A or both B), the payoff matrix is set to be , , and , while if their types are different, the matrix is scaled by a multiplicative factor , and then , and . Evidently, this setting of the payoff matrices can be interpreted as that the efficiency actually is equal to the unity for the interactions between two same-type players, while the efficiency is enhanced to be for two different-type players.
Secondly, after each full cycle of the game, the player compares its own payoffs with those of a randomly chosen neighbor . If the site is not empty, the probability with its strategy changing from to is given by [36] where characterizes the uncertainty related to the strategy adoption process, and and are the payoffs of the player and the player , respectively. In this way, the global density remains constant since no empty sites are ever filled.
In order to characterize the macroscopic behaviors of the system, we introduce a parameter to represent the fraction of cooperators at a given time as follows: where is a total number of sites.
Since we are interested in the long time regime, we define a parameter to represent the average fraction of cooperators as where represents averaging many independent initial states. In this paper, a relative cooperator density is calculated and used to characterize the macroscopic behaviors of the system. Thus, means that the population is fully invaded by the defectors, and , by the cooperators. An intermediate case, for example, , means that cooperators and defectors coexist.
Before showing the simulation results, we would like to analyze how the parameters , , and affect the type of our model. Note when or 1, only one type of players is left and the model returns to the spatial game on the diluted square lattices [28–32]. The introduction of social diversity ceases to affect and the model also returns to the spatial game on the diluted square lattices [28–32] when approaches a unity. Moreover, the introduction of the empty sites ceases to affect and the model returns to the original prisoner’s dilemma based on social diversity [23] when approaches a unity.
Results of MC simulations displayed below are obtained on a square lattice with the periodic boundary conditions and the size of , whereas the stationary density of cooperators is calculated by averaging over MC steps after the sufficiently long transients. Moreover, the final results are averaged over up to 15 independent runs for each set of parameter values in order to assure an appropriate accuracy. The system is updated synchronously.
3. Results and Discussion
First, we present in dependence on for different values of , as shown in Figure 1. For the model returns to the original prisoner’s dilemma based on social diversity [23]. However, in contrast, when some sites on a square lattice are empty, for example, or 0.8, the cooperation level is greatly enhanced for a wide range of . It is reasonable for us to infer that there may be the intermediate values of to enhance the cooperation level for a fixed value of .
In order to examine the effects of the parameter , we study the relative density of cooperators in dependence on for different values of by setting and , as shown in Figure 2. If the occupation fraction is near 0.05, almost all players are isolated and do not change their strategies since there is not any combat at all, and the relative density of cooperators is approximately equal to 0.485. As the density increases, the probability of occurring pairs of occupied sites increases. Irrespective of the value of , the relative density of cooperators decreases from around 0.485, which indicates that some cooperator-defector pairs will become defector-defector pairs. Around , as the number of interacting players increases, the curves for different values of depart: the higher is, the better is for defectors. Still further, there are three interesting cases: the first interesting case happens if , where the relative density of cooperators increases monotonically with the increase of until approaching a unity, which indicates the more players there are, the better it is for cooperators. The second interesting case happens if is in the region , for example, , where the relative density of cooperators increases monotonically with until reaching its maximum value and then sharp decreases. The third interesting case happens if is in the region , for example, , where the behavior is monotonic and the relative density of cooperators decreases monotonically with the increase of until approaching zero. The above results further confirm our previous assertion about some appropriate values for promoting cooperation.
In order to examine the effects of the parameter on the cooperation level, we study the relative density of cooperators in dependence on for different values of by setting and , as shown in Figure 3. If the occupation fraction is near 0.06, almost all players are isolated and do not change their strategies since there is not any combat at all. Irrespective of the values of , the relative density of cooperators is approximately equal to 0.47. As the occupation fraction increases, the probability of occurring pairs of occupied sites increases, and for all the values of , the relative fraction of cooperators decreases from around 0.47, which indicates some cooperator-defector pairs will become defector-defector pairs. Around , as the number of interacting individuals increases, the curves for different values of depart: for , the model returns to the spatial game on the diluted square lattices [28–32], where the relative density of cooperators decreases monotonically with the increase of until approaching zero. For , there are two cases: the first case occurs when is equal to 0.1 or 0.2, where the relative density of cooperators decreases monotonically with the increase of until approaching its minimum value, then increases monotonically with the increase of until approaching its maximum value at . The second case happens when is equal to 0.5, where the relative density of cooperators decreases monotonically with the increase of until approaching its minimum value and then increases monotonically with the increase of until approaching its maximum value around , and finally sharp decreases with the increase of until approaching its minimum value at . The above results indicate that some appropriate values of can promote cooperation.
Besides, for the sake of intuitively understanding the effects of the parameter , some typical snapshots of the system at equilibrium are plotted with respect to different values of when , , and , as shown in Figure 4. Of course, Figure 4 further confirms the conclusions drawn from Figure 3.
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In order to examine the effects of the parameter on the cooperation level, we study independence on for different values of by setting and , as shown in Figure 5. These curves are symmetric around the middle line . For a larger occupation fraction, for example, or 0.9, the fraction of cooperators increases monotonically with the increase of until reaching its maximum value and then decreases with the increase of until the middle point at . Similar non-monotonic behaviors were also found in the previous two-type-player model [23], where each site on the square lattice was occupied. Moreover, the optimum values that maximize the fraction of cooperators are dependent on the region of and are different. For fixed and , the curves turn into the unimodal curves from the bimodal curves with the decrease of . For example, for , there are two maximum values that approximately occur at and 0.72, respectively, but for , there is only one maximum value that approximately occurs at .
In the above discussion, we successively examine the effects of the parameters , , and on the relative density of cooperators, while there is still another parameter not to be discussed. Thus we now focus on how changes with . Results obtained for the different values of by setting and are revealed in Figure 6. For comparison, for the extreme case , the results from [23] are also shown in Figure 6. For the lower occupation densities, for example, , all the isolated cooperator clusters are able to survive for all the values of . But interestingly, as soon as , the relative density of cooperators varies nonmonotonically with the increase of , which indicates that moderately enlarging the gaps among the social ranks can facilitate the cooperation, while exceedingly large or small gaps inhibit cooperation. In addition, although cooperation is possible in a wide range of for , cooperation performs best when . Thus, the two immediate conclusions are (1) cooperation is possible and enhanced if the empty sites are present and (2) the intermediate values of enhance cooperation (unless the density is so low that the game between player and its neighbors does not occur), and exceedingly large or small inhibits cooperation.
In order to investigate the relation between cooperation and social diversity, Perc and Szolnoki [36] introduced the diversity in players' payoffs into the classical spatial prisoner's dilemma game [8] and showed that the diversity could promote cooperation. They also accounted for the observation by the feedback mechanism, in which the players with higher payoffs could dominate their neighbors and eventually form large clusters around them. On the basis of Perc’s work, Li et al. [23] divided the people into two types, that is, A and B. They argued that the types of players are actually dummy, and it is the induced social ranks that play an essential role in the facilitation of cooperation. Besides, they also pointed out that the gaps among ranks depend linearly on the factor of efficiency and the definition of social rank makes sense when the factor of efficiency is much larger than 1.
As to the reasons for some appropriate values for promoting cooperation shown in this paper, referring to the previous works by Li et al. [23], we argue that the empty sites not only induce the changes in the diversified social ranks (or the feedback mechanism) but also prohibit defectors to exploit cooperators. To confirm this argument, we should analyze the varied status of the players in our model, where we define the social rank of a player as the number of its different-type neighbors. When a player plays games with its neighbors, the higher its rank is, the more payoffs obtained in a one-shot game are enhanced by the parameter , and the stronger its ability to collect payoffs. Here, the rank of the player means its ability to collect payoffs. Since the degree of each node on the square lattice is equal to 4, a player may have 0, 1, 2, 3, or 4 different-type neighbors obviously, which determines the player's ranks accordingly. Thus, there are five unequal social ranks in our model. When the focal site is not empty, by calculating the chances of different type-combinations of the focal players located on the square lattice, it is easy to give a so-called rank distribution formula for and as follows: where , respectively, denote the five ranks in the population, denotes the relative fraction of players belonging to rank for fixed and , both and are the combination numbers, and denotes the number of empty sites in a focal player’s neighbors. Obviously, (4) has a symmetry about for a fixed , because the value of should be invariant when we switch each player's type to the other type (meanwhile the value of is changed into ()). For the presentation of the direct observation and impression, we plot the histograms of the rank distribution for different values of by setting in Figure 7.
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By virtue of these histograms, one can find that the different rank distributions in Figure 7 actually correspond to the different trends of the curves in Figure 1. When is slightly smaller than a unity, for example, , as shown in Figure 7(b), most players still occupy the three middle ranks, which are similar to those in Figure 7(a). Thereby, the feedback mechanism in Figure 7(b) is similar to that in Figure 7(a). Nevertheless, under the rank distribution in Figure 7(b), cooperators not only can utilize the interconnectedness between them to form compact clusters, but also can benefit from the dilution that prohibits defectors to exploit them with the same efficiency as on the square lattice fully occupied by players. Thus, the level of cooperation is substantially enhanced in the region of when , as shown in Figure 1. Especially, when further decreases, for example, , as shown in Figure 7(c), the rank distribution obviously changes: most players occupy three lower ranks, while only a few players emerge in two higher ranks, which dramatically weakens the feedback mechanism. Despite that cooperators may still benefit from the dilution, the level of cooperation remarkably decreases by comparison with that for , as shown in Figure 1. When , almost all players occupy three lower ranks and nearly none occupy two higher ranks, as shown in Figure 7(d). It is reasonable for us to infer that the feedback mechanism is further weakened due to the decrease of the higher rank players, which results in a further decrease of , as shown in Figure 1. Moreover, it is found that the smaller is, the more the number of players in lower ranks is, which is consistent with our experience, because a large amount of empty sites reduce the chances of different-type neighbors between the focal player and its neighbors.
Besides, the rank distribution is also affected by for fixed , which was investigated in detail [23]. Since the specific rank distribution induced by parameters and has a significant impact on the evolution of the system, in order to understand comprehensively the influence of and on the rank distribution, the surface charts of the rank distribution dependent on and are plotted in Figure 8. Of course, these results further confirm our previous assertion from the histograms.
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4. Conclusions
In summary, we have extended the model of [23] by introducing some empty sites and endowed this model with more realistic meaning. We have investigated the effects of empty sites on cooperation in the prisoner's dilemma game on the square lattice on the base of social diversity, in which five unequal social ranks are induced by both the setup of the two-type players and empty sites. Our results show that the empty sites dramatically enhance the cooperation level for a wide range of when A players coexist with B players. Moreover, it is found that the maximal cooperation level is obtained when the proportion between the two types of players is quite imbalanced for a larger value of , whereas the maximal cooperation level is obtained when the proportion between the two types is quite balanced for a smaller value of . These results indicate that the optimal collocation between and substantially promotes the cooperation level. It is also found that the cooperation fraction nonmonotonically relies on the factor for a larger occupation fraction, which indicates that the moderate gaps among the social ranks can favor cooperation for a larger occupation fraction. Finally, by calculating the chances of different type-combinations of the players located on the square lattice, we provide a rank distribution formula for and . Based on the above analysis, we find that there is the intermediate region for and that induces five social ranks satisfying certain rank distributions, which is why the intermediate values for and lead to the highest cooperation level at some fixed values of and . We hope this work can contribute to understanding the puzzle of the social cooperation. As for the effect of the temporal aspects of the environment on the interactions between individuals, we will discuss it elsewhere.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
This work was partially supported by the Langfang Teachers College Foundation, China (Grant no. LSZY201204), and the National Science Fund for Distinguished Young Scholars of China (Grant no. 11204214).