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Article

Differential Game-Theoretic Models of Cournot Oligopoly with Consideration of the Green Effect

I.I. Vorovich Institute for Mathematics, Mechanics, and Computer Science, Southern Federal University, 344090 Rostov-on-Don, Russia
*
Author to whom correspondence should be addressed.
Games 2023, 14(1), 14; https://doi.org/10.3390/g14010014
Submission received: 15 December 2022 / Revised: 16 January 2023 / Accepted: 25 January 2023 / Published: 30 January 2023
(This article belongs to the Special Issue Applications of Game Theory with Mathematical Methods)

Abstract

:
We built and investigated analytically and numerically a differential game model of Cournot oligopoly with consideration of pollution for the general case and the case of symmetrical agents. We conducted a comparative analysis of selfish agents’ behavior (a differential game in normal form), their hierarchical organization (differential Stackelberg games), and cooperation (optimal control problem) using individual and collective indices of relative efficiency. The same analysis wasperformed for the models with the green effect when players chose both output volumes and environmental protection efforts. We used the Pontryagin maximum principle for analytical investigation and the method of qualitatively representative scenarios in simulation modeling for numerical calculations. This method allows for reducing the number of computer simulations, providing sufficient precision. As a result of the comparative analysis, systems of collective and individual preferences were obtained.

1. Introduction

A widespread approach to the analysis of game-theoretic models (particularly, differential games) consists in the comparison of results obtained in the cases of selfish players’behavior (differential games in normal form), their hierarchical organization (Stackelberg games), and cooperation (a differential game is reduced to the optimal control problem). For example, a successful illustration of this approach is presented by Zhang et al. [1]. A variant of the approach is described in Ougolnitsky [2]. Basing on Basar and Zhu [3], Cairns and Martinet [4], and some other papers, we proposed in [2] a system of individual and collective indices of the comparative (relative) efficiency for quantitative evaluation of the different ways of organization of economic agents.
A convenient model for the comparative analysis of the different ways of organization of economic agents is Cournot oligopoly (see Maskin and Tirole [5], Geras’kin [6,7], and Algazin and Algazina [8,9]). For example, Xiao et al. [10,11] studied Cournot duopoly with bounded rationality and investigated the equilibria. Raoufinia et al. [12] analyzed open-loop and closed-loop solutions in a Cournot duopoly game with advertising. Al-Khedhairi [13] considered non-trivial Cournot duopoly based on fractal differential equations. Julien [14] investigated Cournot oligopoly with several Stackelberg leaders and followers. A comparison of Cournot and Stackelberg equilibria performed by Zouhar and Zouharova [15].
Together with a standard setup of the oligopoly model that describes a competition of several firms ina market of homogeneous goods, it is interesting to consider the so-called green effect. Usually, the green effect is concerned with supply chains (see Azevedo et al. [16], Fahimnia et al. [17], and Sharma and Jain [18]). It is assumed in this case that the participants of a supply chain invest inthe environmental protection in the processes of production and transportation. The incurred costs are compensated by the willingness of environmentally minded consumers to pay more for products with a green label.
However, the studies of Cournot oligopoly do not include a systematic comparative analysis of the relative profit from the point of view of the whole society and different firms. Besides, the environmental externalities of economic activity and possible environmental protection efforts are not considered.
Thus, the main idea of this paper consists in a comparison of the different ways of organization of economic agents, such as competition, cooperation, and hierarchical control, for differential Cournot oligopoly with pollution dynamics and differential Cournot oligopoly with the green effect. The specific aim consists in building preference systems based on individual and collective indices of relative efficiency.
The contribution of this paper and its novelty areas follows:
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A differential game-theoretic model of Cournot oligopoly with consideration of pollution for the general case and the case of symmetrical agents is built and investigated analytically and numerically.
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A comparative analysis of selfish agents’ behavior (a differential game in normal form), their hierarchical organization (differential Stackelberg games), and cooperation (optimal control problem) using individual and collective indices of relative efficiency is conducted.
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We performed the same analysis for the models with the green effect when players chose both output volumes and environmental protection efforts.
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We constructed systems of collective and individual preferences.
In Section 2, we characterize the materials and methods of the investigation. In Section 3, we build and investigate a differential game model of Cournot oligopoly for the selfish behavior of players, their hierarchical organization, and cooperation. The case of symmetrical players and the general case are considered. We applied the Pontryagin maximum principle for analytical investigation and simulation modeling for numerical calculations. We used a system of individual and collective indices of relative efficiency for the quantitative comparison of the obtained results. In Section 4, similar work is performed for the modelswith the green effect when players invest in environmental protection. Section 5 concludes the paper.

2. Materials and Methods

The main analytical instrument of the investigation is the well-known Pontryagin maximum principle [19]. For numerical calculations, we used an original method of qualitatively representative scenarios in simulation modeling [20]. The idea consists in choosing a relatively small number of control scenarios that providea sufficiently precise description of the dynamics of the controlled system. For the substantiation of sufficiency, two conditions are used, namely the conditions of internal and external stability. Suppose an initial set of scenarios is chosen. It is internally stable if for any two scenarios from this set, the respective payoffs of the players differ essentially. It is externally stable if for any feasible scenario that does not belong to this set, we can find a scenario from this set such that the respective payoffs of the players are close. The value of precision of such approximations is chosen empirically and should not exceed 10% from the typical values of payoffs.
For quantitative comparative evaluation of the different ways of organization of economic agents (information structures of the respective game-theoretic models) from the point of view of both the whole society and separate agents, we introduced a system of relative efficiency indices [2], namely:
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collective indices of relative efficiency;
S C I N E = i = 1 n J i N E J C ;     S C I S T = i = 1 n J i S T J C ;   S C I i S T = i = 1 n J i i S T J C
The values J i S T   and   J i I S T determine the payoffs of the i-th player in the Stackelberg and inverse Stackelberg games, respectively, when the i -th player is the leader. Any player can become the leader; in our examples, it is the first player.
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individual indices of relative efficiency.
K i N E = min x N E J i N E ( x ) J C / n ;   K i S T = J i S T J C / n ;     K i I S T = J i I S T J C / n
The payoffs are supposed to be non-negative.
We proposed a mathematical model that is a dynamic version of Cournot oligopoly with consideration of environmental pollution. The main approach to its identification is an expert estimate using available real data. There were five main parameters in the model: (1) the concentration of pollutants in the environment in the initial moment of time, (2) a coefficient of the pollutants’ emission during production, (3) a coefficient of decay of the pollutants in the environment, (4) a maximal output for any firm, and (5) a cost coefficient for each firm. For the numerical identification of their values, we used the following reasonings. As a pollutant, we can consider carbon monoxide (CO). It is toxic, and its admissible concentration in production premises is 20 mg/m3 during a working day or 50 mg/m3 during an hour or 100 mg/m3 during 30 min. Based on this, the concentration of pollutants in the environment in the initial moment of time varied from 1 to 50 mg/m3. The coefficient of the pollutants’ emission during production depends on the production volume. For example, a coke chemical plant emits annually about 2000 tons of carbon monoxide. Based on this, the value of pollutants’ emission varied from 0.1 to 30 tons per year; the maximal output for any firm varied from 5 to 70,000 tons per year, and the cost coefficient for each firm varied from 1 to 50. The decay of many pollutants is slow; for example, carbon monoxide decays only in the presence of a catalyst. Thus, we varied the coefficient of decay of the pollutants from 0.1 to 30 kg per year. In addition, discounting was considering in the model, and a discount factor was taken to be equal to 0.004 that corresponds to moderate inflation. The modeling was conducted at an interval of 1200 days.

3. Differential Game Model of Cournot Oligopoly with Consideration of Pollution

Let us consider a dynamic version of Cournot oligopoly with consideration of environmental pollution and the linear equation of dynamics:
J i = 0 T e r t α 1 ( a c i x ¯ ( t ) ) x i ( t ) d t e r T α 2 y ( T ) m a x  
                            0 x i ( t ) ,   t [ 0 , T ] ,     i = 1 , , n   ;
d y d t = i = 1 n k i x i ( t ) m y ( t ) ,       y ( 0 ) = y 0 .
Here, { 1 , 2 , , n } is a set of firms (agents, players) competing in the manner of Cournot oligopoly in a market of homogeneous goods;   J i is the i -th player’s profit in time T ; x ¯ ( t ) = i = 1 n x i ( t ) ;   x i is the output volume of the i -th firm (its strategy); the expression in parentheses in Formula (1) determines the price for the produced good, depending on the demand that is conversely proportional to the total output volume; α 1   and   α 2 are dimensioned coefficients that provide the fitness of dimension (for simplicity, they are assumed to be equal to 1); y ( t ) is the volume of pollutants in the environment (a state variable); k i is the coefficient of emission in the production of the i -th firm; a is the demand parameter;   c i is the cost coefficient of the i-th firm; m is the coefficient of pollution decay; r is the discount factor; and T is the length of the game. The agents’ interaction is described by their strategies and the final value of the state variable in the moment of time T .
In the case of symmetrical agent s   ( k i , = k ;   c i , = c ; x i , = x ) ,   the model in Formulas (1)–(3) takes the form
J = 0 T e r t ( a c n x ( t ) ) x ( t ) d t e r T y ( T )   m a x
0 x ( t ) ,   t [ 0 , T ] ,
d y d t = k n x m y ( t ) ,       y ( 0 ) = y 0 .
We supposed that all players use open-loop piecewise continuous strategies. The agents may be selfish, so we have a differential game in normal form with Nash equilibrium as its solution. In addition, the agents may cooperate, so the game is reduced to the optimal control problem. Finally, a hierarchical organization is possible that is formalized by differential Stackelberg and inverse Stackelberg games [21,22].
Let us first consider a selfish behavior of the agents and investigate the symmetrical model in Formulas (4)–(6) using the Pontryagin maximum principle [19]. The Hamilton function for each player has the form
H ( x , u , λ ) = ( a c n x ( t ) ) x ( t ) + λ ( k n x ( t ) m y ( t ) ) ,
where λ ( t ) is a conjugate variable. We obtain
H x = a c 2 n x + k n λ = 0
and
      x N E = a c + k n λ 2 n   .      
Here, 2 H   x 2 = 2 n < 0 . Therefore, the found value x N E maximizes the Hamilton function if a c + k n λ > 0 , or the value belongs to the domain of feasible strategies, Formula (5). Otherwise, the point of maximum coincides with the lower bound of the set of feasible strategies of the agent. A conjugate variable is determined from the boundary value problem
λ t = r λ ( t ) H y = ( r + m ) λ ( t ) ;   λ ( T ) = 1 .
Then,
λ i N E = λ N E ( t ) = e ( r + m ) ( T t ) ,
and Formula (7) is a maximizer of the Hamilton function if a c k n e ( r + m ) ( T t ) > 0 .
Thus, we obtain
x N E = m a x ( 0 , ( k e ( r + m ) ( T t ) 2 + ( a c ) / ( 2 n ) ) )
If   a c k n e ( r + m ) ( T t ) > 0     f o r   t > 0 ,     then   x N E ( t ) = a c 2 n k 2 e ( r + m ) ( T t ) y N E ( t ) = y 0 e m t + k ( a c ) 2 m ( 1 e m t ) k 2 n 2 ( r + 2 m ) ( e ( r + m ) ( T t ) e m t ( r + m ) T ) J N E = ( a c ) 2 4 n r ( 1 e r T ) k 2 n 4 ( r + 2 m ) ( e r T e 2 ( r + m ) T )
These calculations show that Nash equilibrium exists and is unique.
Using Formulas (8) and (9), we conducted numerical calculations for different input data sets in the case of symmetrical agents. We realized about 100 numerical calculations. We varied the following parameters: n from 2 to 40, a from 5 to 70 , c from 1 to 50, m from 0.1 to 30, k from 0.1 to 30, and y 0 from 1 to 50. The input data are presented in Table 1, and the agents’ payoffs for the input data from Table 1 for T   = 1200 and r = 0.001 are presented in Table 2. Here and elsewhere, NE stands for Nash equilibrium, C for cooperative solution, and S T and I S T for Stackelberg and inverse Stackelberg games, respectively.
In the case of arbitrary agents, the Hamilton function for the i -th player is
H i ( x i ( t ) , u i ( t ) , λ i ( t ) ) = ( a c i x ¯ ( t ) ) x i ( t ) + λ i ( t ) ( i = 1 n k i x i ( t ) m ( t ) y ( t ) )
Then,
H i x i = a c i j = 1 n x j x i + k λ i = 0 ;     i = 1 , 2 , , n
and 2 H i x 2 = 2 n < 0 . Therefore, the solutions of Formula (10) maximize the Hamilton function if they belong to the sets of feasible strategies. For conjugate variables, Formula (8) is applied.
Solving the system of equations in Formula (10), we obtain
x i N E = m a x ( 0 , ( k i e ( r + m ) ( T t ) + a n c i + j = 1 ; j i n c j ) / ( n + 1 ) )   ;     i = 1 , 2 , , n .                            
Let us consider the case k i e ( r + m ) ( T t ) + a n c i + j = 1 ; j i n c j > 0 ;   t > 0 .
Substitute Formula (11) in the equation of dynamics and solve it by the method of variation of parameters:
y N E = y 0 e m t + 1 e m t ( n + 1 ) m i = 1 n k i ( a n c i + j = 1 ; j i n c j ) k i 2 n ( n + 1 ) ( r + 2 m ) ( e ( r + m ) ( T t ) e m t ( r + m ) T )
Then
J i N E = ( a n c i + j = 1 ; j i n c j ) a c i ( n + 1 ) r ( 1 e r T ) k i ( a c i ) ( n + 1 ) m ( e r T e ( r + m ) T ) + k i ( n + 1 ) 2 m j = 1 n ( a n c i + k = 1 ; j k n c k ) ( e r T e ( r + m ) T ) + 1 ( n + 1 ) 2 ( e 2 ( r + m ) T e r T ) j = 1 n k j ( k i r + 2 m 1 m ( a n c i + k = 1 ; i k n c k ) ) ( a n c i + k = 1 ; i k n c k ) 1 ( n + 1 ) 2 r ( 1 e r T ) j = 1 n ( a n c j + k = 1 ; j k n c k ) e r T y N E ( T ) .
The input data are presented in Table 3, and the results for three arbitrary agents at T = 1200   and   r = 0.001 for the input data from the Table 3 are presented in Table 4.
When all agents cooperate we obtain an optimal control problem:
J c = i = 1 n 0 T e r t ( a c i j = 1 n x j ( t ) ) x i ( t ) d t n e r T y ( T ) m a x
0 x i ( t ) ,   t [ 0 , T ] ,     i = 1 , , n   ;     d y c d t = i = 1 n k i x i ( t ) m y c ( t ) ,       y c ( 0 ) = y 0
In the symmetrical case ( k i = k ;   c i = c ; i = 1 , 2 , .. , n ) , the problem takes the form
J c = 0 T e r t ( a c x ( t ) ) x ( t ) d t n e r T y ( T ) m a x 0 x ( t ) ,   t [ 0 , T ] , d y C d t = k x ( t ) m y C ( t ) ;   y C ( 0 ) = y 0 ;     x ( t ) = i = 1 n x i ( t ) .
Similarto the case considered earlier, we obtain λ C ( t ) = n e ( r + m ) ( T t ) :
x c ( t ) = m a x ( 0 , ( k n e ( r + m ) ( T t ) 2 + a c 2 ) )
If k e ( r + m ) ( T t ) + a c > 0 ;   t > 0 , then
x C ( t ) = a c 2 k n 2 e ( r + m ) ( T t ) y C ( t ) = y 0 e m t + k ( a c ) 2 m ( 1 e m t ) k 2 n 2 ( r + 2 m ) ( e ( r + m ) ( T t ) e m t ( r + m ) T ) J C = ( a c ) 2 4 r ( 1 e r T ) k 2 n 2 4 ( r + 2 m ) ( e r T e 2 ( r + m ) T ) y ( T ) e r T
In Table 2, in the third and fourth columns, the results of calculations in the case of cooperation for the input data from Table 1 are presented.
When arbitrary agents cooperated, the solution was found numerically [23,24] using the method of qualitatively representative scenarios in simulation modeling [20]. The initial sets of qualitatively representative scenarios were taken as sets that consisted of three elements: 0, a big number (10,000 as a specific example), and their average value. All elements of the initial set were checked for completeness and redundancy [20], and it was reduced or extended with new elements by necessity. The calculation results are presented in Table 4.
Now, let us consider the case of hierarchical relations between agents in two versions of the information structure. In a Stackelberg game, one of the agents (e.g., the first one) becomes the leader (she). She chooses and reports to the other agents (followers) her open-loop strategy x 1 ( t ) .
The followers play a differential game in normal form. The best response of the followers to the leader’s strategy is defined as Nash equilibrium in this game. We solved n 1 optimal control problems (1)–(3) for i = 1 , 2 , , n . A solution of each problem was found using the Pontryagin maximum principle, similar to Formulas (10) and (11), and had the form
x i * ( t ) = m a x ( 0 , x i 0 x 1 n )   ;     i = 2 , 3 , , n
where i = 2 , 3 , , n ;
x i 0 ( t ) = 1 n ( a + j = 2 ; j i n c j ( n 1 ) k i ( n 1 ) c i ) + 1 n ( j = 2 ; j i n k j + ( n 1 ) k i ) e ( r + m ) ( T t ) .
Substitute Formula (13) into Formulas (1) and (3) and solve the problem in Formulas (1) and (3) using the Pontryagin maximum principle for i = 1 . An optimal strategy of the first player has the form
x 1 * ( t ) = m a x ( 0 , x 1 0 )   ,    
where
  x 1 0 ( t ) = a 2 n 2 c 1 + 1 2 e ( r + m ) ( T t ) i = 2 n ( j = 2 ; j i n k j ( n 1 ) k i ) 1 2 i = 2 n ( j = 2 ; j i n c j ( n 1 ) c i ) k 1 n 2 e ( r + m ) ( T t )
Thus, in Stackelberg equilibrium, the first player (leader) chooses her strategy, Formula (14). Given the leader’s strategy, other players choose their strategies according to Formula (13). Given all players’ strategies, the state variable is determined using the solution of Formula (3) and the payoffs are determined using Formula (1).
In an inverse Stackelberg game [21,22] based on the model in Formulas (1)–(3), the leader reports to each follower her strategy, with feedback on their control
x 1 i 0 ( t ) = { x 1 i R ( t ) ,       i f   x i ( t ) = x i R ( t ) ,     i = 2 , 3 , , n x 1 i P ( t ) ,           o t h e r w i s e   .                                  
If a follower refuses to cooperate with the leader, then she punishes the follower using the punishment strategy x 1 i P = ( x 12 P , x 13 P , , x 1 n P ) , which according to Formula (13) has the form ( i = 2 , 3 , , n ) .
x 1 i P ( t ) = arg min x 1 i 0 ( ( ( n 1 ) k i j = 2 ; j i n k j ) e ( r + m ) ( T t ) x 1 i + a j = 2 ; j i n c j ( n 1 ) c 1 i )
Then, a guaranteed result of the i -th follower is equal to
L i = m a x { x j N E } j = 2 n J i ( { x 1 k P } k = 2 n , x 2 , x 3 , , x n ) = J i ( { x 1 k P } k = 2 n , 0 , 0 , , 0 ) = e r T y ( T ) = e r T ( y 0 + k 1 T x 1 i P ( T ) )
If the followers cooperate with the leader, then she chooses a reward strategy x 1 i R = ( x 12 R , x 13 R , , x 1 n R ) . The reward strategies ( x 12 R , x 13 R , , x 1 n R ) are found as solutions of the optimal control problem
J 1 = 0 T e r t ( a c 1 x ¯ ( t ) ) x 1 ( t ) d t e r T y ( T ) m a x { x i ( t ) } i = 1 n
0 x i ( t ) ,   t [ 0 , T ] ,   i = 1 , 2 , , n ;
d y d t = i = 1 n k i x i ( t ) m y ( t ) ,       y ( 0 ) = y 0
J i = 0 T e r t ( a c i x ¯ ( t ) ) x i ( t ) d t e r T y ( T ) > L i ;     i = 2 , 3 , , n .
A solution of the problem in Formulas (15) and (16) was found numerically with computer simulation. The condition in Formula (16) provides that a reward is always more profitable for the followers than punishment. The payoffs of all players in the Stackelberg and inverse Stackelberg games are presented in Table 4.
The values of individual and collective indices of relative efficiency for different information structures are given in Table 5. In the last row of Table 5, the average values of the collective and individual efficiency indices on the set of simulation experiments are presented. Thus, we obtained the following preference systems:
society: C N E I S T S T ;
agent-leader:   I S T S T C N E ;
agent-follower:   C N E S T I S T .
As expected, cooperation is always preferable for the whole society and for followers. However, for the leader, the information structure of the inverse Stackelberg game is the most profitable as a rule. That is why the struggle for leadership arises often.

4. A Model with Consideration of the Green Effect

Now, the model takes the form
J i = 0 T ( e r t ( a c i x ¯ ( t ) + α g ¯ ( t ) ) x i ( t ) β i g i 2 ( t ) ) d t e r T y ( T ) m a x
0 x i ( t ) ,   0 g i ( t ) , t [ 0 , T ] ,     i = 1 , , n   ;
d y d t = i = 1 n ( k i x i ( t ) γ i g i ( t ) ) m y ( t ) ,       y ( 0 ) = y 0
where g i ( t ) characterizes green efforts of the i -th firm, α is the coefficient of demand increasing due to the green effect, β i is the green effort coefficient, and γ i is the coefficient of additional decreasing of the pollution due to green efforts.
In the case of symmetrical agents, the model takes the form
J = 0 T ( e r t ( a c n x ( t ) + α n g ( t ) ) x ( t ) β g 2 ( t ) ) d t e r T y ( T ) m a x
0 x ( t ) ,   0 g ( t ) , t [ 0 , T ] ,      
d y d t = n ( k x ( t ) γ g ( t ) m y ( t ) ,       y ( 0 ) = y 0
The agents’ strategies contain two control actions (functions x i ( t ) and g i ( t ) ). The Hamilton function for each player in the symmetrical model in Formulas (20)–(22) has the form
H ( x , g , y , λ ) = ( a c n x ( t ) + α n g ( t ) ) x ( t ) β g 2 ( t ) + λ ( n ( k x ( t ) γ g ( t ) ) m y ( t ) ) .
We obtain
H x = a c 2 n x + α n g + λ n k = 0 ;   H g = a n x 2 β g γ n λ = 0 .
So, if 4 n β α 2 n 2   0 , then
g 0 ( t ) = α n x 0 γ n λ 2 β ;     x 0 ( t ) = ( a c ) 2 β γ n 2 α λ + 2 β λ k n   4 n β α 2 n 2
If 4 n β α 2 n 2 = 0 and γ n λ 2 β ( a c + λ k n   ) , then the maximum is attained on the bound of the set of feasible controls (at least one of the optimal controls is not internal).
If 4 n β α 2 n 2 = 0 and γ n λ = 2 β ( a c + λ k n ) , then g 0 ( t ) = α n x 0 γ n λ 2 β ;   x 0 ( t ) is an arbitrary function that belongs to the set of feasible strategies, for example, x 0 ( t ) 0   t 0 . Denote
A = ( a c ) 2 β   4 n β α 2 n 2 ;   B = γ n 2 α λ + 2 β λ k n   4 n β α 2 n 2 ;     C = α n A 2 β ; D = α n β γ n 2 β
Given λ ( t ) = e ( r + m ) ( T t ) , if 4 n β α 2 n 2 0 , then
x 0 ( t ) = A e ( r + m ) ( T t ) B ;   g 0 ( t ) = C e ( r + m ) ( T t ) D .    
Notice that 2 H x 2 = 2 n ;   2 H g 2 = 2 β ; 2 H x g = α n .
Therefore, the found value is a maximizer if a sufficient condition Δ = 4 n β α 2 n 2 > 0 is true and the value belongs to the set of feasible strategies, i.e., for t 0 ; A e ( r + m ) ( T t ) B ;   C e ( r + m ) ( T t ) D . If at least one of the inequalities
A e ( r + m ) ( T t ) B ;   C e ( r + m ) ( T t ) D ;   4 n β α 2 n 2 > 0
is false, then in dependence on the input model parameters, the maximum is obtained in one of the boundary points
( 0 , γ m 2 β e ( r + m ) ( T t ) )   or   ( a c n k e ( r + m ) ( T t ) 2 n , 0 )
Thus,
( x * , g * ) = { ( x 0 , g 0 )           i f     A e ( r + m ) ( T t ) B ;   C e ( r + m ) ( T t ) D ;   4 n β α 2 n 2 > 0   ( 0 , γ m 2 β e ( r + m ) ( T t ) )   o r   ( a c n k e ( r + m ) ( T t ) 2 n , 0 )               o t h e r w i s e .
The state variable was calculated using the method of parameter variation. Given the inequalities in Formula (18), it is explained by the formula
y ( t ) = y 0 e m t + E m ( 1 e m t ) F r + 2 m ( e ( r + m ) ( T t ) e m t ( r + m ) T )
when E = n k A γ n C ; F = n k B γ n D . The payoffs are equal to
J = G r ( 1 e r T ) H m ( e r T e ( r + m ) T ) + I r + 2 m ( e r T e 2 ( r + m ) T ) + y ( T ) e r T ,
where
G = ( a c n A + α n C ) β D 2 ;   H = ( a c n A + α n C ) B + A ( α n D n B ) 2 β C D ;       I = B ( n B + α n D ) β D 2 .
In the case of cooperation, the model takes the form
J = i = 1 n J i = i = 1 n 0 T ( ( a c i x ¯ ( t ) + α g ¯ ( t ) ) x i ( t ) β g i 2 ( t ) ) d t n e r T y ( T ) m a x 0 x i ( t ) ,   0 g i ( t ) , t [ 0 , T ] ,   i = 1 , 2 , , , , n .     d y d t = i = 1 n ( k i x i ( t ) γ i g i ( t ) ) m y ( t ) ,       y ( 0 ) = y 0
The maximum is obtained by the values
x ( t ) = ( x 1 ( t ) , x 2 ( t ) , , x n ( t ) ) ;   g ( t ) = ( g 1 ( t ) , g 2 ( t ) , , g n ( t ) )
Nash equilibrium was calculated numerically using computer simulation [22,23]. The input data are given in Table 6, and the results for symmetrical agents with consideration of the green effect are presented in Table 7 for the input data from Table 6.
In the case of arbitrary agents (model in Formulas (17)–(19)), the Nash equilibria for selfish behavior and cooperative solutions were calculated numerically using computer simulation. In Table 8 the input data are given, and in Table 9 the results for three arbitrary agents at T = 1200   and   r = 0.001 for the input data from Table 8 are presented.
Now consider a hierarchical setup with consideration of the green effect. Let a specific agent (principal) maximize the functional
J 0 = 0 T e r t ( ( a x ¯ ( t ) + α g ¯ ( t ) ) x ¯ ( t ) i = 1 n ( c i x i ( t ) + β i g i 2 ( t ) ) ) d t n e r T y ( T ) m a x
by controls g i ( t ) ; i = 1 , 2 , , n .
The other agents’ payoff functionals retain the form Formula (17), but now, the maximization is conducted only by the controls x i ( t ) . The equation of dynamics has the form Formula (19). Control constraints are of the form Formula (18) again.
In the Stackelberg game, similarto the preceding case, we obtained the solution in the game of agents in the form of Formula (25).
In Table 10, the values of the indices of collective and individual relative efficiency with consideration of the green effect are presented. The last row of Table 10 contains the average values of the respective indices. The indices of individual efficiency were calculated only for the case of cooperation.
In this case, we obtained the same preference system for the whole society and the followers:
C N E S T I S T .
This preference system remains the same as the system without consideration of the green effect. However, the consideration of the green effect makes the agents’ interests more diverse, and the whole economic system becomes less (for some input data sets, essentially less) compatible. In this case, for the whole society, cooperation is much better than other ways of organization.

5. Conclusions

The proposed system of individual and collective indices of the relative efficiency of the ways of organization [2] was used for the analysis of differential game-theoretic models of Cournot oligopoly with consideration of the green effect and without it. For calculation of the indices, we applied averaging on the set of simulation experiments. The numerical calculations showed that the introduced indices allow for evaluation of the average efficiency of different ways of organization (information structures) and for practical recommendations on improving system compatibility.
The preference systems for the whole society and separate agents are contradictory. Cooperation is more profitable for the society and followers. However, the leader prefers a hierarchy in the form of an inverse Stackelberg game that advocates for struggle for leadership. Moreover, for non-symmetrical agents, cooperation may be either more profitable than selfish behavior or vice versa (Table 10, column 3). Notice also that the consideration of the green effect makes cooperation much more profitable (up to 50%) for the whole society and followers.
In the future, we plan to study static and dynamic game-theoretic models of Cournot oligopoly in the form of characteristic function. In addition, the models with a network structure both in normal form and in the form of a characteristic function will be considered. At last, model identification will be precisely performed.

Author Contributions

Conceptualization, review, methodology, and formal analysis and investigation G.O.; investigation, A.U. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

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Table 1. Input data in the case of symmetrical agents.
Table 1. Input data in the case of symmetrical agents.
Example n a c k m y 0
1530151210
2520151210
3517151210
4510151210
5540151210
61020151210
752051210
8520155210
9520150.2210
10520151110
11520151510
12520151230
1352015122
145201511010
1552015522
16520155510
1752015115
18220151210
192020151210
20230151210
2122051210
222201511010
2322015121
24220151220
2522015125
26102051210
27101051210
28103051210
291020510210
30102050.2210
3110205121
32102051220
3310205123
341030151210
351020153210
36102051615
37102015210
3810201010210
Table 2. Payoffs for different information structures for symmetrical agents.
Table 2. Payoffs for different information structures for symmetrical agents.
No. N E C
J * y ( T ) J c y ( T )
113,4033.8567,0153.85
21476073800
3223011150
41476073800
537,2745.6186,3725.6
67453.1274503.12
713,4183.1267,0903.12
81483074150
914910.2274550.22
1014901.2574501.25
1114910.2574550.25
1214910.6374550.63
1314910.6374550.63
1414910.1374550.13
151483074150
161488074400
1714901.2574501.25
183727174541
19371.5074300
2033,5473.567,0943.5
2133,5473.567,0943.5
2237280.274560.2
233727174541
243727174541
253727174541
2667092.567,0902.5
27744.93.174493.1
2818,6376.1186,3706.1
296648066,4800
3067100.767,1000.7
3167092.567,0902.5
3267092.567,0902.5
3367092.567,0902.5
3467092.567,0902.5
35740074000
3667090.8367,0900.83
3710,7500107,5000
382920029,2000
Table 3. Input data in the case of arbitrary agents ( n = 3 ).
Table 3. Input data in the case of arbitrary agents ( n = 3 ).
Example a c 1 c 2 c 3 k 1 k 2 k 3 my0
12510155123210
2251015510.53210
3251153113210
4251153153210
52520155115210
63051520115210
72510515123210
82551510541210
925515100.212210
1025115510.10.3110
112520151010.50.50.510
1225515110.11230
1325515111322
14251151010.50.10.110
1525515150.2122
1625515150.51510
1725515114215
181810155143210
19301015144210
2025115510.10.8210
2135153010.10.5210
223510153010.110.110
234530152012321
2445301520120.5220
254530151512125
26301052132210
273015523135210
283015528133210
2930155121010.2210
303015570.210.5210
31302053120.521
32302053120.1220
3330105210.5323
34301151810.50.2210
35301152030.50.8210
3630152010.51615
37305120521210
Table 4. Payoffs of arbitrary agents for different information structures.
Table 4. Payoffs of arbitrary agents for different information structures.
No.NESTISTC
J 1 J 2 J 1 J 2 J 1 J 2 J C
116,769185625,342102529,855854110,567
216,765185224,878103227,856987110,211
3119,27719,073136,56515,456142,87812,378217,345
4119,29219,082136,54515,467143,11112,176217,431
516,753184719,654118721,878108333,962
6186,3887456192,3214231195,2763765203,477
716,77791,33222,32185,34424,12380,433110,367
891,328185998,7881098103,287944111,213
991,327186197,8781112100,433952111,214
10131,49914,599138,76611,232145,3889321198,376
11745174549233698711,653601282,943
1250,39014,60456,57812,34359,72111,488199,432
1350,38814,59856,69912,51161,24511,298199,173
14164,6035934171,2343767174,8323077181,326
1550,38314,59657,65510,76759,7278999198,234
1650,39214,60657,68810,82259,2119122198,321
1750,40614,60858,02210,82459,3449211198,411
18477310,733623193567113873374,987
192666131,4963457125,6765234120,924186,333
20131,50314,604147,34411,288156,3447455198,211
21334,659193,906348,656180,344356,745175,901711,548
22186,37267,093202,37855,344213,48853,977322,121
237438186,3718433180,4339123177,843262,321
247443186,3718511180,4339211177,855262,377
2516,761150,95819,431144,87721,322140,234320,432
26364054,336524447,865586746,904173,231
2712,602209,42517,355195,87719,742192,511250,375
2824,156250,79731,866241,82235,805238,091363,543
29296131,5222033125,6495386124,034147,786
30665102,056234594,545412993,532169,111
3136,074107,64745,23394,56554,00591,714306,342
3236,076107,64844,211100,45650,05698,455306,435
33364054,338834348,23410,27347,431172,768
34268,3801186272,345756274,611690276,356
35286,5602666294,3441213298,0531054305,421
36201,58796,618223,18783,423228,76980,521343,221
3796,601201,577103,421192,344113,591185,732344,234
Table 5. Indices of relative efficiency for different information structures.
Table 5. Indices of relative efficiency for different information structures.
Example N E S T I S T
S C I K 1 N E / K 2 N E / K 3 N E SCI K 1 S T / K 2 S T / K 3 S T SCI K 1 I S T / K 2 I S T / K 3 I S T
10.990.45/0.05/2.480.940.69/0.03/2.10.910.81/0.02/1.9
20.990 45/0.05/2.480.930.68/0.03/2.090.910.76/0.03/1.95
30.981.64/0.26/1.050.981.89/0.21/0.850.971.97/0.17/0.78
40.981.64/0.26/1.050.981.88/0.21/0.840.971.97/0.17/0.76
50.991.48/0.16/1.330.951.73/0.1/1.00.951.93/0.1/0.81
60.982.74/0.1/0.10.992.84/0.06/0.060.992.88/0.06/0.06
70.990.46/2.48/0.050.980.6/2.32/0.030.960.7/2.19/0.03
80.982.48/0.05/0.460.992.67/0.03/0.030.992.79/0.03/0.03
90.982.48/0.05/0.460.992.67/0.03/0.030.992.79/0.03/0.03
100.991.99/0.22/0.760.982.1/0.17/0.690.982.2/0.14/0.58
110.980.27/0.27/2.430.920.33/0.25/2.180.890.42/0.22/2.04
120.980.76/0.22/1.990.960.83/0.19/1.860.930.84/0.11/1.24
130.980.76/0.22/1.990.960.83/0.19/1.860.930.84/0.11/1.24
140.982.72/0.1/0.150.992.83/0.06/0.10.992.79/0.05/0.07
150.990.76/0.22/1.990.980.87/0.16/1.90.960.9/0.14/1.84
160.990.76/0.22/1.990.980.87/0.16/1.90.960.9/0.14/1.84
170.990.76/0.22/1.990.980.87/0.16/1.90.960.9/0.14/1.84
180.980.19/0.43/2.30.940.25/0.37/2.190.890.28/0.35/2.02
190.990.04/2.11/0.810.950.06/2.02/0.760.920.08/1.95/0.73
200.991.99/0.22/0.750.972.22/0.17/0.530.982.36/0.13/0.47
210.991.41/0.82/0.750.981.47/0.76/0.70.971.5/0.76/0.67
220.991.74/0.62/0.620.981.89/0.52/0.530.991.99/0.5/0.49
230.980.09/2.13/0.770.950.1/2.1/0.70.940.1/2.0/0.68
240.980.09/2.13/0.770.950.1/2.1/0.70.940.1/2.0/0.68
250.990.16/1.41/1.410.970.18/1.36/1.370.940.2/1.31/1.32
260.990.06/0.94/1.960.90.09/0.83/1.780.870.1/0.81/1.71
270.940.15/2.51/0.320.940.2/2.35/0.270.940.24/2.3/0.26
280.990.2/2.06/0.710.970.26/2.0/0.660.970.3/1.97/0.65
290.980.01/2.67/0.290.940.04/2.55/0.240.950.11/2.52/0.22
300.980.01/1.81/1.110.910.04/1.68/1.020.910.07/1.66/1.00
310.980.35/1.01/1.540.940.44/0.92/1.470.950.53/0.9/1.42
320.990.35/1.05/1.540.940.43/0.98/1.420.950.49/0.96/1.4
330.990.06/0.94/1.960.940.14/0.84/1.850.940.18/0.82/1.81
340.992.91/0.01/0.050.992.96/0.01/0.010.992.98/0.01/0.01
350.982.87/0.02/0.140.992.89/0.01/0.060.992.93/0.01/0.05
0.991/0.87/1.090.961.11/0.8/0.960.971.17/0.77/0.96
Table 6. Input data for symmetrical agents with consideration of the green effect.
Table 6. Input data for symmetrical agents with consideration of the green effect.
Example n a c k m y 0 α βγ
15301512100.0110.1
25201512100.0110.1
35171512100.0110.1
45101512100.0110.1
55401512100.0110.1
610201512100.0110.1
7520512100.0110.1
85301512100.00110.1
95301512100.510.1
105301512100.520.1
115301512100.5100.1
125301512100.550.01
135301512100.550.5
145301512100.510.5
15520155220.510.5
16520155220.50.50.5
17520155220.510.5
18520155220.110.5
1920201512100.110.1
202301512100.110.1
21220512100.110.1
2222015110100.110.1
23220151210.110.1
242201512200.110.1
252201512200.510.1
262201512200.10.50.1
272201512200.110.5
282201512200.510.5
292201512200.30.50.1
302201512200.810.3
31102051210.110.1
321020512200.110.1
33102051230.110.1
3410301512100.110.1
3510201532100.110.1
361020516150.410.3
Table 7. Payoffs for different information structures for symmetrical agents with consideration of the green effect.
Table 7. Payoffs for different information structures for symmetrical agents with consideration of the green effect.
No. N E C
J y ( T ) J y ( T )
113,4173.169,0123.3
214900.676111
3238011950
41491075670
537,2755.6189,4555.6
6745075700
713,4183.1670,8453.1
813,4163.1670,9223.1
919,515499,0114.5
1015,9013.580,1123.7
1113,8493.270,2382.8
1214,3103.371,9873.7
1314,3102.871,9873.4
1419,5171.198,3891.5
152160011,1000
1639640199,100
172160011,1000
181502077320
19391079110
2033,7133.568,3223.5
2133,7160.768,3241.1
2237460.276230.4
233745176231.4
243745176231.3
2514591.130271.4
263764176551.2
2737450.876231.3
2842590.889151.3
294095183121.3
3054801.111,0111.2
3168792.469,1142.6
3268792.469,1142.6
3368792.469,1142.6
3468792.469,1142.6
35759077010
3611,1820.3113,5320.5
Table 8. Input data for three arbitrary agents with consideration of the green effect.
Table 8. Input data for three arbitrary agents with consideration of the green effect.
No. a c 1 c 2 c 3 k 1 k 2 k 3 m y 0 β 1 β 2 β 3 γ 1 γ 2 γ 3 α
130125101152101520.010.50.10.01
2203755122105120.10.50.010.01
3173551242102130.20.10.050.01
4101211252101510.50.10.20.01
54010251512101320.20.10.30.01
6205351242102510.30.10.010.01
7205521352101250.20.10.050.01
83010751522103210.50.10.70.001
93010551242101340.20.10.010.5
103087101152102150.30.10.20.5
11306101015321010450.50.10.10.5
1230105101422105110.10.010.050.5
1330101051262105230.20.50.10.5
143035101512101510.30.50.050.5
1520324525221850.20.50.10.5
1640255524220.5120.050.50.70.5
1740451053322120.50.050.50.80.5
184071010521222120.20.50.10.1
194010551522101250.50.10.20.1
203051021242102110.30.10.30.1
21205361152103150.20.10.50.1
222028113410101530.20.10.50.1
2320514125211720.50.10.050.1
24205621142202120.30.10.20.1
25203521212201110.50.10.20.5
26205851552200.50.520.50.10.30.1
27205121522201510.10.50.050.1
28205281342201150.050.10.50.5
29405561142200.5510.20.050.10.3
30409541252202130.10.30.30.8
31405116153211230.50.10.20.1
324051101242201310.30.10.50.1
33255105135235130.20.10.050.1
345015551522101320.30.10.20.1
Table 9. Payoffs for different information structures with the green effect.
Table 9. Payoffs for different information structures with the green effect.
No. N E S T / I S T
J 1 J 2 J 3 J 0 J 1 J 2 J 3
133432745502617/2911150/1442067/1715400/350
27263149541204/1813467/404127/114609/538
3542277581848/1217313/266174/159360/237
4147203147427/852127/112172/143127/112
51043285139886890/8122861/6222381/17653648/3288
63426528341370/3282296/211466/352608/388
743243213311557/2136249/177249/1771059/899
8572186314672960/3172390/3111556/11861015/886
9534123723113214/3542306/176961/7211947/1783
1083498712372471/2712701/524821/604949/745
1123236726722724/30061862/1562431/378431/378
1252526315252622/2879325/2561972/1568325/256
1349549526482596/2870316/278316/2781963/1672
14155421673723029/37651136/7561739/1453154/144
155667838221567/1872408/278500/389658/465
162845345618696401/70212061/17652909/27531432/1299
17231138928835833/60231844/15673337/3098652/525
182391298114565659/57621781/15662595/23851284/1098
192656243124316322/65442298/19872012/18772012/1877
20225441116633183/32111742/1567159/1541283/1076
218096713221294/1277610/577470/455214/197
22114518812712303/25341008/899110/1021198/934
233728247391391/1512200/177580/562611/578
2432424213021474/1634252/213162/1381061/812
257405698241836/2195649/587427/397760/674
26 4511788421208/1411354/302128/98727/621
2741576212531785/1784204/199585/568995/982
2855116751312233/2451517/4621607/1523114/94
292231223139127608/79231983/16421983/17653642/3277
30652159834264942/5342474/4141331/11893137/2873
312434125339546637/70122001/1763949/8213687/3456
32396228119426712/67123467/34342502/2488743/727
3372118915422092/2112642/623141/1281307/1198
3416217234376111,063/11,6511062/8216684/6431 3318/3176
Table 10. Indices of relative efficiency of the players for different information structures with consideration of the green effect.
Table 10. Indices of relative efficiency of the players for different information structures with consideration of the green effect.
Example N E S T / I S T
S C I K 1 / K 2 / K 3 S C I K 1 L / K 2 F / K 3 F /
10.890.21/2.1/0.350.56/0.470.1/1.33/0.26 /0.09/1.1/0.23
20.951 04/0.45/1.360.57/0.50.67/0.18/0.87/0.58/0.16/0.77
30.961.11/0.57/1.190.58/0.450.64/0.36/0.74/0.55/0.33/0.49
40.830.73/1.01/0.730.71/0.610.63/0.86/0.63/0.56/0.71/0.56
50.740.29/0.8/1.120.64/0.530.24/0.67/1.02 /0.18/0.5/0.92
60.850.48/0.91/1.170.64/0.440.41/0.65/0.85/0.3/0.5/0.54
70.920.55/0.55/1.680.66/0.440.31/0.31/1.34/0.22/0.22/1.13
80.940.37/1.2/0.950.64/0.490.25/1.0/0.65/ 0.2/0.77/0.57
90.880.35/0.8/1.50.69/0.580.2/0.62/1.26/0.11/0.47/1.15
100.780.63/0.75/0.940.63/0.470.53/0.62/0.72/0.4/0.46/0.57
110.851.62/0.43/0.470.63/0.541.3/0.3/0.29 /1.01/0.26/0.26
120.80.34/1.72/0.340.57/0.450.21/1.29/0.21/0.17/1.02/0.17
130.80.33/0.33/1.740.57/0.470.2/0.2/1.29/0.18/0.18/1.10
140.750.86/1.2/0.210.56/0.430.49/0.96/0.08/0.42/0.8/0.08
150.90.71/0.98/1.030.65/0.450.45/0.62/0.82 /0.35/0.49/0.58
160.810.81/0.98/0.530.61/0.550.62/0.83/0.41/0.5/0.78/0.37
170.750.73/1.23/0.280.62/0.540.61/1.06/0.21/0.5/0.98/0.17
180.850.89/1.11/0.540.7/0.630.65/0.97/0.48/0.58/0.89/0.41
190.820.87/0.8/0.770.69/0.630.75/0.66/0.66/0.65/0.62/0.62
200.751.17/0.21/0.860.55/0.480.9/0.08/0.66/0.81/0.08/0.56
210.841.13/0.93/0.450.6/0.570.85/0.65/0.3 /0.8/0.63/0.27
220.971.27/0.21/1.410.86/0.721.12/0.12/1.33/1.0/0.11/1.04
230.720.42/0.92/0.820.52/0.490.22/0.65/0.68/0.2/0.63/0.65
240.790.41/0.31/1.640.62/0.490.32/0.2/1.34/0.27/0.17/1.03
250.910.95/0.73/1.060.78/0.690.83/0.55/0.97/0.75/0.51/0.86
260.880.81/0.32/1.510.72/0.610.63/0.23/1.3/0.54/0.18/1.11
270.920.47/0.87/1.430.68/0.660.23/0.67/1.13/0.23/0.65/1.12
280.990.69/2.1/0.160.94/0.870.65/2.02/0.14/0.58/1.92/0.12
290.910.73/0.73/1.280.83/0.730.65/0.65/1.19/0.54/0.58/1.07
300.790.27/0.67/1.430.59/0.620.19/0.55/1.31/0.17/0.49/1.21
310.830.8/0.41/1.290.72/0.660.66/0.31/1.21/0.58/0.27/1.13
320.681.04/0.74/0.250.59/0.590.92/0.66/0.2/0.91/0.66/0.19
330.820.72/0.19/1.550.7/0.650.65/0.14/1.31/0.63/0.13/1.2
340.830.32/1.44/0.750.73/0.690.21/1.32/0.66/0.16/1.28/0.63
0.840.71/0.85/0.960.66/0.570.58/0.69/0.95/0.49/0.58/0.72
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Ougolnitsky, G.; Usov, A. Differential Game-Theoretic Models of Cournot Oligopoly with Consideration of the Green Effect. Games 2023, 14, 14. https://doi.org/10.3390/g14010014

AMA Style

Ougolnitsky G, Usov A. Differential Game-Theoretic Models of Cournot Oligopoly with Consideration of the Green Effect. Games. 2023; 14(1):14. https://doi.org/10.3390/g14010014

Chicago/Turabian Style

Ougolnitsky, Guennady, and Anatoly Usov. 2023. "Differential Game-Theoretic Models of Cournot Oligopoly with Consideration of the Green Effect" Games 14, no. 1: 14. https://doi.org/10.3390/g14010014

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