Noncooperative Oligopoly in Markets with a Cobb-Douglas Continuum of Traders Giulio Codognato and Ludovic A. Julien

April 2013 n. 1/2013

Noncooperative Oligopoly in Markets with a Cobb-Douglas Continuum of Traders∗ Giulio Codognato†and Ludovic A. Julien‡ April 2013

Abstract In this paper, we reconsider two models of noncooperative oligopoly in general equilibrium proposed by Busetto et al. ((2008), (2011)): a version of the Shapley’s window model for mixed exchange economies `a la Shitovitz and its reformulation `a la Cournot-Walras. We introduce the assumption that preferences of the traders belonging to the atomless part are represented by Cobb-Douglas utility functions. This assumption permits us to prove the existence of a Cournot-Nash equilibrium of the Shapley’s window model - called Cobb-Douglas-CournotNash equilibrium - without introducing further assumptions on atoms’ endowments and preferences previously used by Busetto et al. (2011). Then, we show that the set of the Cobb-Douglas-Cournot-Nash equilibrium allocations coincides with the set of the Cournot-Walras equilibrium allocations. Journal of Economic Literature Classification Numbers: C72, D51. Keywords: strategic market games, noncooperative oligopoly, atoms, atomless part. ∗ We would like to thank Francesca Busetto for the comments and suggestions contained in her report. Giulio Codognato gratefully acknowledges financial support from MIUR (PRIN 20103S5RN3). † Dipartimento di Scienze Economiche e Statistiche, Universit` a degli Studi di Udine, Via Tomadini 30, 33100 Udine, Italy, and EconomiX, Universit´e de Paris Ouest Nanterre la D´efense, 200 Avenue de la R´epublique, 92001 Nanterre Cedex, France. ‡ LEG, Universit´e de Dijon, 2 boulevard Gabriel, 21066, Dijon Cedex, France, and EconomiX, Universit´e de Paris Ouest Nanterre la D´efense, 200 Avenue de la R´epublique, 92001 Nanterre Cedex, France.

1

1

Introduction

Noncooperative oligopoly in interrelated markets has been modeled within two main approaches. The first is the strategic market game approach, initiated by Shapley and Shubik (see also Dubey and Shubik (1978), Postlewaite and Schmeidler (1978), Okuno et al. (1980), Mas-Colell (1982), Sahi and Yao (1989), Amir et al. (1990), Peck et al. (1992), Dubey and Shapley (1994), among others). In this class of models, all traders behave strategically and prices are determined according to non-Walrasian pricing rules. The second is the Cournot-Walras approach, initiated by Gabszewicz and Vial (1972) for economies with production (see also Roberts and Sonnenschein (1977), Roberts (1980), Mas-Colell (1982), Dierker and Grodal (1986), among others), and by Codognato and Gabszewicz (1991) for pure exchange economies (see also Codognato and Gabszewicz (1993), d’Aspremont et al. (1997), Gabszewicz and Michel (1997), Shitovitz (1997), Julien and Tricou (2005), (2009), among others). In this class of models, some agents behave strategically while others behave competitively and prices are determined according to the Walrasian pricing rule. Strategic agents determine their strategies as in the Cournot game (see Cournot (1838)) taking into account the Walrasian price correspondence. Both classes of models aim at studying the working and the consequences of market power in a general equilibrium framework. More recently, Busetto et al. (2008), (2011) introduced two models of noncooperative oligopoly in general equilibrium, inspired by a strategic market game originally proposed by Lloyd S. Shapley and known as Shapley’s window model. This model was further analyzed by Sahi and Yao (1989) in exchange economies with a finite number of traders, and Codognato and Ghosal (2000) in exchange economies with an atomless continuum of traders. More precisely, Busetto et al. (2011), taking inspiration from a seminal paper by Okuno et al. (1980), proved the existence of a Cournot-Nash equilibrium of the Shapley’s window model associated with an exchange economy `a la Shitovitz (1973), i.e., with atoms and an atomless part. Instead, Busetto et al. (2008) provided a respecification `a la Cournot-Walras of this mixed exchange economy assuming that atoms behave `a la Cournot while the atomless part behaves `a la Walras. They showed, by an example, that the set of the Cournot-Nash equilibrium allocations does not coincide with the set of the Cournot-Walras equilibrium allocations in a one-stage setting. Nevertheless, they introduced a reformulation of the Shapley’s model as a two-stage game, where the atoms move in the first stage and the atomless sector moves in the second stage, and showed that the set of the Cournot-Walras equilib2

rium allocations coincides with a specific set of subgame perfect equilibrium allocations of this two-stage game. In this paper, we reconsider these two models under the assumption that preferences of the traders belonging to the atomless part are represented by Cobb-Douglas utility functions. Beyond their tractability to compute solutions in theoretical models, Cobb-Douglas utility functions will turn out very useful to establish the relationships among the equilibrium concepts studied in this paper. We first show the existence of a Cobb-Douglas-Cournot-Nash equilibrium - i.e., a Cournot-Nash equilibrium where the strategies of the traders belonging to the atomless part depend on the parameters of their Cobb-Douglas utility functions - under the following further assumptions: (i) each trader is endowed with a strictly positive amount of at least one commodity and each commodity is held, in the aggregate, by the atomless part; (ii) atoms’ utility functions are continuous, strongly monotone, and quasi-concave; (iii) traders’ utility functions are jointly measurable. Busetto et al. (2011) proved the existence of a more general Cournot-Nash equilibrium by using less restrictive assumptions on the atomless part’s endowments and preferences. In particular, they assumed that the atomless part has continuous, strongly monotone, and quasi-concave preferences without requiring that it holds, in the aggregate, each commodity. Nevertheless, our proof is not merely a special case of theirs: indeed, following Sahi and Yao (1989), they imposed the hypothesis that there exists at least two atoms with endowments and indifference curves contained in the strict interior of the commodity space. This hypothesis can be removed in our context, therefore, our proof allows us to deal with cases where all atoms have corner endowments and indifference curves which cross the boundary of the commodity space. Then, following Busetto et al. (2008), we provide a respecification `a la Cournot-Walras of our model and we prove that, under the assumptions (i)-(iii) mentioned above, the set of the Cobb-Douglas-Cournot-Nash equilibrium allocations coincides with the set of the Cournot-Walras equilibrium allocations. This result contrasts with the example provided by Busetto et al. (2008) mentioned above which shows that it may not hold if preferences of the traders belonging to the atomless part are not represented by Cobb-Douglas utility functions. The paper is organized as follows. In Section 2, we present the mathematical model. In Section 3, we show the existence of the Cobb-DouglasCournot-Nash equilibrium. Section 4 is devoted to the Cournot-Walras equilibrium. Section 5 aims at studying the relationship between the Cobb3

Douglas-Cournot-Nash and the Cournot-Walras equilibrium. Section 6 concludes.

2

The mathematical model

We consider a pure exchange economy, E, with large traders, represented as atoms, and small traders, represented by an atomless part. The space of traders is denoted by the measure space (T, T , µ), where T is the set of traders, T is the σ-algebra of all µ-measurable subsets of T , and µ is a real valued, non-negative, countably additive measure defined on T . We assume that (T, T , µ) is finite, i.e., µ(T ) < ∞. This implies that the measure space (T, T , µ) contains at most countably many atoms. Let T1 denote the set of atoms and T0 = T \ T1 the atomless part of T . A null set of traders is a set of measure 0. Null sets of traders are systematically ignored throughout the paper. Thus, a statement asserted for “each” trader in a certain set is to be understood to hold for all such traders except possibly for a null set of traders. The word “integrable” is to be understood in the sense of Lebesgue. l . There are l different commodities. A commodity bundle is a point in R+ An assignment (of commodity bundles to traders) is an integrable function l . There is a fixed initial assignment w, satisfying the following x: T → R+ assumption. R Assumption 1. w(t) > 0, for each t ∈ T , T0 w(t) dµ À 0. Furthermore, as in Sahi and Yao (1989), we can assume, for convenience, R j (t) dµ = 1, j = 1, . . . , l. An allocation is an assignment x for which that w T R R x(t) dµ = T T w(t) dµ. The preferences of each trader t ∈ T are described by a utility function l → R. We assume that atoms’ preferences are represented by utility ut : R+ functions which satisfy standard continuity, monotonicity, and concavity assumptions. We do not assume, as Busetto et al. (2011) did, that there exist atoms whose indifference curves lie in the strict interior of the commodity space. On the other hand, we introduce the crucial assumption that the traders belonging to the atomless part have Cobb-Douglas utility functions. l → R is continuous, strongly monotone, and quasiAssumption 2. ut : R+ 1 l concave, for each t ∈ T1 , ut (x) = x1α (t) · · · xlα (t) , for each t ∈ T0 and j l , where α: T → Rl for each x ∈ R+ 0 ++ is a function such that α (t) > 0, Pl j = 1, . . . , l, j=1 αj (t) = 1, for each t ∈ T0 .

4

N l ) denote the Borel σ-algebra of Rl . Moreover, let T Let B(R+ B + denote the σ-algebra generated by the sets E × F such that E ∈ T and F ∈ B. l Assumption 3. u : T × R + → R given by u(t, x) = ut (x), for each t ∈ T N l , is T and for each x ∈ R+ B-measurable. l . We define, for each p ∈ Rl , a A price vector is a vector p ∈ R+ + correspondence ∆p : T → P(Rl ) such that, for each t ∈ T , ∆p (t) = {x ∈ l : px = pw(t)}, a correspondence Ψ : T → P(Rl ) such that, for each R+ p l : for all y ∈ ∆ (t), u (x) ≥ u (y)}, and finally t ∈ T , Ψp (t) = {x ∈ R+ p t t a correspondence Xp : T → P(Rl ) such that, for each t ∈ T , Xp (t) = ∆p (t) ∩ Ψp (t). A Walras equilibrium of E is a pair (p∗ , x∗ ), consisting of a price vector ∗ p and an allocation x∗ , such that x∗ (t) ∈ Xp∗ (t), for each t ∈ T . l , it is possible to define the atomBy Assumption 2, for each p ∈ R++ l such that less part’s Walrasian demands as a function x0 (·, p) : T0 → R+ 0 x (t, p) = Xp , for each t ∈ T0 . It is immediate to verify that x0j (t, p) = P αj (t) li=1 pi wi (t) , j = 1, . . . , l, for each t ∈ T0 . The following proposition pj shows that this function is integrable.

Proposition 1. Under Assumptions 1, 2, and 3, the function x0 (·, p) is l . integrable, for each p ∈ R++ l . The restriction of w to T is integrable as w is Proof. Let p ∈ R++ 0 integrable. Now, we prove that α is a measurable function. Consider a l . Let u0 (·, y) denote the restriction of u(·, y) commodity bundle y ∈ R++ to T0N . The function u(·, y) must be measurable as, by Assumption 3, u(·, ·) is T B-measurable (see Theorem 4.48 in Aliprantis and Border (2006), p. 152). Then, the function u0 (·, y) is also measurable. Suppose that α l such that α−1 (O) is not measurable. Then, there is an open set O ∈ R+ l l is not a µ-measurable set. Let f : R → R++ be a function such that f (v) = (y1v1 , . . . , ylvl ), for each v ∈ Rl . f (O) is an open set as f is a homeomorphism. Suppose that τ ∈ α−1 (O). Then, f (α(τ )) ∈ f (O). But then, τ ∈ (u0 (·, y))−1 (f (O)). Therefore, α−1 (O) ⊂ (u0 (·, y))−1 (f (O)). Suppose that τ ∈ (u0 (·, y))−1 (f (O)). Moreover, suppose that τ ∈ / α−1 (O). 0 Then, α(τ ) ∈ / O. But then, u (τ, y) ∈ / f (O), a contradiction. Therefore, (u0 (·, y))−1 (f (O)) ⊂ α−1 (O). Then, α−1 (O) = (u0 (·, y))−1 (f (O)). But then, α−1 (O) is µ-measurable as u0 (·, y) is measurable, a contradiction. Therefore, α is P measurable. Hence, x0 (·, p) is integrable as it is measurable

and x0j (t, p) <

l i=1

pi wi (t) , pj

j = 1, . . . , l, for each t ∈ T0 . 5

3

Cobb-Douglas-Cournot-Nash equilibrium

We introduce now the strategic market game, Γ, associated with E, following the reformulation of the Shapley’s window model proposed by Busetto et al. l2 be a vector such that b = (b , b , . . . , b (2011). Let b ∈ R+ 11 12 ll−1 , bll ). A 2 l strategy correspondence is a correspondence B : T → P(R+ ) such that, for Pl l2 : i each t ∈ T , B(t) = {b ∈ R+ j=1 bij ≤ w (t), i = 1, . . . , l}. A strategy 2

selection is an integrable function b : T → Rl , such that, for each t ∈ T , b(t) ∈ B(t). For each t ∈ T , bij (t), i, j = 1, . . . , l, represents the amount of commodity i that trader t offers in exchange for commodity R j. Given ¯ = ( bij (t) dµ). a strategy selection b, we define the aggregate matrix B T Moreover, we denote by b \ b(t) a strategy selection obtained by replacing b(t) in b with b ∈ B(t). With a slight abuse of notation, b \ b(t) will also represent the value of the strategy selection b \ b(t) at t. Then, we introduce two further definitions (see Sahi and Yao (1989)). Definition 1. A nonnegative square matrix A is said to be irreducible if, for every pair (i, j), with i 6= j, there is a positive integer k = k(i, j) such (k) (k) that aij > 0, where aij denotes the ij-th entry of the k-th power Ak of A. Definition 2. Given a strategy selection b, a price vector p is market clearing if l l X X l ¯ ij = pj ( ¯ ji ), j = 1, . . . , l. p ∈ R++ , pi b b (1) i=1

i=1

By Lemma 1 in Sahi and Yao (1989), there is a unique, up to a scalar ¯ is irreducible. Then, multiple, price vector p satisfying (1) if and only if B we denote by p(b) a function which associates with each strategy selection ¯ is b the unique, up to a scalar multiple, price vector p satisfying (1), if B irreducible, and is equal to 0, otherwise. Given a strategy selection b and a price vector p, consider the assignment determined as follows: xj (t, b(t), p) = wj (t) −

l X

bji (t) +

i=1 j

l X i=1

j

x (t, b(t), p) = w (t), otherwise, j = 1, . . . , l, for each t ∈ T .

6

bij (t)

pi l , , if p ∈ R++ pj

According to this rule, given a strategy selection b and the function p(b), the traders’ final holdings are determined as follows: x(t) = x(t, b(t), p(b)), for each t ∈ T . It is straightforward to show that the assignment corresponding to the final holdings is an allocation. This reformulation of the Shapley’s window model for mixed exchange economies allows us to define the following concept of Cournot-Nash equilibrium. ¯ ˆ such that B ˆ is irreducible is a CournotDefinition 3. A strategy selection b Nash equilibrium of Γ if ˆ ˆ ≥ ut (x(t, b ˆ \ b(t), p(b ˆ \ b(t)))), ut (x(t, b(t), p(b))) for each b ∈ B(t) and for each t ∈ T . In order to define the notion of Cobb-Douglas-Cournot-Nash equilibrium l2 such that b0 (t) = wi (t)αj (t), i, j = we consider a function b0 : T0 → R+ ij 0 (t) ∈ B(t), for each t ∈ T , as 1, . . . , l, for each t ∈ T0 . Then, we have b 0 P wi (t)αj (t) ≥ 0, i, j = 1, . . . , l, and lj=1 wi (t)αj (t) = wi (t), i = 1, . . . , l, for each t ∈ T0 . The following proposition shows that the function b0 is integrable. Proposition 2. Under Assumptions 1, 2, and 3, the function b0 is integrable. Proof. b0 is measurable as the restriction of w to T0 is measurable and we know, from the proof of Proposition 1, that α is measurable. Then, b0 is integrable as b0ij (t) < wi (t), i, j = 1, . . . , l, for each t ∈ T0 . We can now provide the definition of a Cobb-Douglas-Cournot-Nash equilibrium of Γ. ˆ is a Cobb-Douglas-Cournot-Nash equiDefinition 4. A strategy selection b ˆ librium of Γ if it is a Cournot-Nash equilibrium of Γ and b(t) = b0 (t), for each t ∈ T0 . The rest of this section is devoted to prove the existence of a CobbDouglas-Cournot-Nash equilibrium. To this end, we first need to introduce an auxiliary game, which we call Γ1 , where only the atoms act strategically, taking b0 as given. We will also need to show that Lemmas 3 and 4 in Sahi and Yao (1989) can readapted to our framework. The game Γ1 has, mutatis 7

mutandis, the same structure as Γ. We can now establish a relationship between Γ1 and Γ which will be used in the proof of the existence theorem. l2 be a function such that b1 (t) ∈ B(t), for each t ∈ T . Let b1 : T1 → R+ 1 R R R P P b1 is integrable as t∈T1 t b1 (t) dµ ≤ t∈T1 t w(t) dµ = T1 w(t) dµ < ∞. Then, b1 is a strategy selection of Γ1 . Given a strategy selection b1 of Γ1 , l2 be a function such that b10 (t) = b1 (t), for each t ∈ T , let b10 : T → R+ 1 and bR10 (t) = b0 (t),R for each t ∈ RT0 . Then, b10R is a strategyR selection of Γ as T1 b1 (t) dµ + T0 b0 (t) dµ ≤ T1 w(t) dµ + T0 w(t) dµ = T w(t) dµ < ∞. Consider an atom τ ∈ T1 . Given a strategy selection b10 , consider a vector ¯b ∈ B(τ ). Suppose that ¯bii 6= b10 ii (τ ), for at least a pair (i, i), and ¯bij = b10 (τ ), for the remaining pairs (i, j). Then, it is straightforward to ij verify that p(b10 ) = p(b10 \ ¯b(τ )). Therefore, as in Sahi and Yao (1989), we can assume, for convenience and without loss of generality, that, given P i a strategy selection b10 , lj=1 b10 ij (t) = w (t), i = 1, . . . , l, for each t ∈ T1 . Then, given a strategy selection b10 , the corresponding R aggregate matrix ¯ 10 is row-stochastic. Moreover, B ¯ 10 is irreducible as B T0 w(t) dµ À 0 and α(t) À 0, for each t ∈ T0 . We can now provide the definition of a Cournot-Nash equilibrium of Γ1 . ˆ 1 is a Cournot-Nash equilibrium of Γ1 Definition 5. A strategy selection b if ˆ 1 (t), p(b ˆ 10 )) ≥ ut (x(t, b ˆ 1 \ b(t), p(b ˆ 10 \ b(t)))), ut (x(t, b for each b ∈ B(t) and for each t ∈ T1 . The following argument adapts to our framework the setting of Lemmas 3 and 4 in Sahi and Yao (1989), which we use to prove the existence theorem. Consider an atom τ ∈ T1 . Given a strategy selection b10 , let D be a matrix ¯ 10 − b10 (τ )µ(τ ), i, j = 1, . . . , l. Then, from (1), we have such that dij = b ij ij l X

l X j 10 pi (b10 )(dij + b10 (τ )µ(τ )) = p (b )( (dji + b10 ij ji (τ )µ(τ )), j = 1, . . . , l,

i=1

i=1

from which we obtain −

l X

l X

b10 ji (τ )+

i=1

pi (b10 ) b10 ij (τ ) j 10

i=1

p (b )

Pl

i=1 dji

=

µ(τ )

Pl

i=1 dij



µ(τ )

pi (b10 ) , j = 1, . . . , l. pj (b10 )

Then, j

10

10

j

x (τ, b (τ ), p(b )) = w (τ ) +

Pl

i=1 dji

µ(τ ) 8

Pl −

i=1 dij

µ(τ )

pi (b10 ) , j = 1, . . . , l, pj (b10 )

from which we obtain j

10

Pl

10

(µ(τ ))x (τ, b (τ ), p(b )) = 1 −

i 10 i=1 dij p (b ) , pj (b10 )

j = 1, . . . , l.

(2)

It is possible to show that Lemmas 3 and 4 in Sahi and Yao (1989) still hold for an atom τ when their matrices C and A are replaced, respectively, with ¯ 10 , and their Equation (14) is replaced with (2). Lemmas 3 and 4 D and B together imply that the “best response set” of an atom in Γ1 is nonempty, convex, and compact. We can now prove the existence of a Cobb-Douglas-Cournot-Nash equilibrium of Γ. Theorem 1. Under Assumptions 1, 2, and 3, there exists a Cobb-Douglasˆ Cournot-Nash equilibrium of Γ, b. Proof. The assumption that µ(T ) < ∞ implies that T1 may be either finite or countably infinite. We shall consider the case where T1 contains countably infinite atoms as the argument we use for this caseQholds, a fortiori, when it contains a finite number of atoms. Let Φ : Q t∈T1 B(t) → Q 1 ) = {b1 ∈ B(t) be a correspondence such that Φ(b t∈T1 t∈T1 B(t) : 1 1 b (t) ∈ Φt (b Q ), for each t ∈ T1 } where, for each t ∈ T1 , the correspondence Φt : t∈T1 B(t) → B(t) is such that Φt (b1 ) = argmax{ut (x(t, b1 \ Q l2 b(t), p(b10 \ b(t)))) : b ∈ B(t)}. t∈T1 R+ is a locally convex Hausdorff Q space as it is a metric space. t∈T1 B(t) is a nonempty, convex, and comQ l2 as B(t) is nonempty, convex, and compact, for pact subset of t∈T1 R+ Q each t ∈ T1 . Consider a trader τ ∈ T1 . For each b1 ∈ t∈T1 B(t), Φτ (b1 ) is nonempty, convex, and closed, as Lemma 4 in Sahi and Yao (1989) holds in our framework. Moreover, Φτ is upper hemicontinuous by the Berge Maximum Theorem (see Theorem 17.31 in Aliprantis and Border (2006), p. 570). Then, Φτ has a closed graph, by the Closed Graph Theorem (see Theorem 17.11 in Aliprantis and Border (2006), p. Q 561) as t∈T1 B(t) is compact and Φτ is upper hemicontinuous and closedvalued. But then, the correspondence Φ has nonempty, convex values, and a closed graph. Therefore, by the Kakutani-Fan-Glicksberg Theorem (see Theorem 17.55 in Aliprantis and Border (2006), p. 583) there exists a ˆ 1 of Φ, which is a Cournot-Nash equilibrium b ˆ 1 of Γ1 . Let fixed point b 10 ˆ ˆ ˆ b be a strategy selection of Γ such that b(t) = b (t), for each t ∈ T . 10 ¯ ¯ ˆ is irreducible as B ˆ is irreducible. Consider a trader τ ∈ T1 . Then, B ˆ ), p(b))) ˆ ˆ \ b(τ ), p(b ˆ \ b(τ )))), for each b ∈ B(τ ), uτ (x(τ, b(τ ≥ uτ (x(τ, b 9

ˆ 1 is a Cournot-Nash equilibrium of Γ1 . Consider a trader τ ∈ T0 . as b Pl j i ˆ i (τ ) ˆ ), p(b)) ˆ ∈ X ˆ (τ ) as xj (τ, b(τ ˆ ), p(b)) ˆ = α (τ ) i=1 p (b)w x(τ, b(τ , j = ˆ pj (b)

p(b)

ˆ \ ¯b(τ ), p(b ˆ\ 1, . . . , l. Suppose that there exists ¯b ∈ B(τ ) such that uτ (x(τ, b ¯b(τ )))) > uτ (x(τ, b(τ ˆ ), p(b))). ˆ ˆ \ ¯b(τ )) = It is immediate to verify that p(b ¯ ˆ ˆ ˆ p(b). Let x ¯ = x(τ, b \ b(τ ), p(b)). Then, it is straightforward so show that ˆ ), p(b))) ˆ x ¯ ∈ ∆p(b) (τ ). But then, uτ (¯ x) > uτ (x(τ, b(τ and x ¯ ∈ ∆p(b) ˆ ˆ (τ ), a ˆ ˆ ≥ ut (x(t, b ˆ \ b(t), p(b ˆ \ b(t)))), contradiction. Therefore, ut (x(t, b(t), p(b))) ˆ for each b ∈ B(t) and for each t ∈ T . Hence, b is a Cobb-Douglas-CournotNash equilibrium of Γ.

4

Cournot-Walras equilibrium

In this section, we describe the concept of Cournot-Walras equilibrium proposed by Busetto et al. (2008). The atomless part has Walrasian del , defined in Section mands represented by the function x0 (·, p) : T0 → R+ 2 2. Consider now the atoms’ strategies. Let e ∈ Rl be a vector such that e = (e11 , e12 , . . . , ell−1 , ell ). A strategy correspondence is a correspondence 2 2 E : T1 → P(Rl ) such that, for each t ∈ T1 , E(t) = {e ∈ Rl : eij ≥ Pl 0, i, j = 1, . . . , l; j=1 eij ≤ wi (t), i = 1, . . . , l}. A strategy selection is an 2

integrable function e : T1 → Rl such that, for each t ∈ T1 , e(t) ∈ E(t). For each t ∈ T1 , eij (t), i, j = 1, . . . , l, represents the amount of commodity i that trader t offers in exchange for commodity j. We denote by e \ e(t) a strategy selection obtained by replacing e(t) in e with e ∈ E(t). With a slight abuse of notation, e \ e(t) will also denote the value of the strategy selection e \ e(t) at t. Given a strategy selection e, consider the following equation: Z x0j (t, p) dµ + T0

l Z X i=1

T1

eij (t) dµ

pi = pj

Z wj (t) dµ + T0

l Z X i=1

T1

eji (t) dµ, (3)

j = 1, . . . , l. When defining their notion of Cournot-Walras equilibrium, Busetto et al. (2008) assumed the existence of a market clearing price vector satisfying (3). Moreover, as market clearing price vectors may not be unique, they had to define their equilibrium concept with respect to an arbitrary selection among market clearing prices. The following proposition shows that, thanks

10

to the assumption that traders belonging to the atomless part have CobbDouglas preferences, there exists a unique, up to a scalar multiple, price l vector p ∈ R++ which satisfies Equation (3). Proposition 3. Under Assumptions 1, 2, and 3, for each strategy selection l e, that there exists a unique, up to a scalar multiple, price vector p ∈ R++ which satisfies Equation (3). 2

l be a function Proof. Consider a strategy selection e. Let e10 : T → R+ such that e10 (t) = e(t), for each t ∈ T1 , and e10 (t) = b0 (t), for each t ∈ T0 . Then, e10 is integrable by the sameR argument used for the function b10 . ¯ 10 = ( e10 (t) dµ). E ¯ 10 is irreducible by the Define the aggregate matrix E T ij 10 ¯ . (3) can be written as same argument used for the matrix B l X i=1

l Z X = pj ( ( i=1

Z p( i

Z i

j

w (t)α (t) dµ +

T0

T1

eij (t) dµ)

Z

wj (t)αi (t) dµ +

T0

T1

eji (t) dµ)), j = 1, . . . , l.

Then, (3) can be rewritten as l X i=1

j pi ¯ e10 ij = p (

l X

¯ e10 ji ), j = 1, . . . , l.

(4)

i=1

By Lemma 1 in Sahi and Yao (1989), there is a unique, up to a scalar l ¯ 10 is irreducible. Hence, multiple, price vector p ∈ R++ satisfying (4) as E l there exists a unique, up to a scalar multiple, price vector p ∈ R++ which satisfies Equation (3). We denote by p(e) a function which associates, with each strategy selection e, the unique, up to a scalar multiple, price (3). It is R vector p satisfying R straightforward to verify that p(e0 ) = p(e00 ) if T1 e0 (t) dµ = T1 e00 (t) dµ. For l denote a function each strategy selection e, let x1 (·, e(·), p(e)) : T1 → R+ such that x1j (t, e(t), p(e)) = wj (t) −

l X i=1

eji (t) +

l X i=1

eij (t)

pi (e) , pj (e)

(5)

j = 1, . . . , l, for each t ∈ T1 . Given a strategy selection e, taking into account the structure of the traders’ measure space, Proposition 3, and 11

Equation (3), it is straightforward to show that the function x(t) such that x(t) = x1 (t, e(t), p(e)), for all t ∈ T1 , and x(t) = x0 (t, p(e)), for all t ∈ T0 , is an allocation. At this stage, we are able to define the concept of Cournot-Walras equilibrium. Definition 6. A pair (˜ e, x ˜), consisting of a strategy selection ˜ e and an allocation x ˜ such that x ˜(t) = x1 (t, ˜ e(t), p(˜ e)), for each t ∈ T1 , and x ˜(t) = x0 (t, p(˜ e)), for each t ∈ T0 , is a Cournot-Walras equilibrium of E if ut (x1 (t, ˜ e(t), p(˜ e))) ≥ ut (x1 (t, ˜ e \ e(t), p(˜ e \ e(t)))), for each e ∈ E(t) and for each t ∈ T1 .

5

Cobb-Douglas-Cournot-Nash and CournotWalras equilibrium

Since either the bids of the traders belonging to the atomless part, at a Cobb-Douglas-Cournot-Nash equilibrium, and their Walrasian demands, at a Cournot-Walras equilibrium, depend on the the parameters of their CobbDouglas utility functions, we are lead to raise the question whether these two equilibrium notions are equivalent in our framework. The following theorem provides a positive answer to our question. Indeed, it shows that the set of the Cobb-Douglas-Cournot-Nash equilibrium allocations coincides with set of the Cournot-Walras equilibrium allocations. ˆ is a Cobb-DouglasTheorem 2. Under Assumptions 1, 2, and 3, (i) if b Cournot-Nash equilibrium of Γ, then there is a strategy selection ˆ e such that 1 10 ˆ ˆ the pair (ˆ e, x ˆ), where x ˆ(t) = x(t, b(t), p(b)) = x (t, ˆ e(t), p (ˆ e)), for each t ∈ ˆ ˆ = x0 (t, p10 (ˆ T1 , and x ˆ(t) = x(t, b(t), p(b)) e)), for each t ∈ T0 , is a CournotWalras equilibrium of E; (ii) if (˜ e, x ˜) is a Cournot-Walras equilibrium of E, ˜ of Γ such that then there is a Cobb-Douglas-Cournot-Nash equilibrium b ˜ ˜ for each t ∈ T . x ˜(t) = x(t, b(t), p(b)), ˆ be a Cobb-Douglas-Cournot-Nash equilibrium of Γ. Let ˆ Proof. (i) Let b e ˆ be a strategy selection such that ˆ e(t) = b(t), for each t ∈ T1 . Then, p(ˆ e) = 10 ¯ ¯ ˆ as E ˆ satisfies Equation (1). But then, it is straightforˆ =B ˆ and p(b) p(b) ˆ ˆ = x1 (t, ˆ ward to verify that x(t, b(t), p(b)) e(t), p(ˆ e)), for each t ∈ T1 , and 0 ˆ ˆ x(t, b(t), p(b)) = x (t, p(ˆ e)), each t ∈ T0 . Suppose that there is a trader τ ∈ T1 and a strategy e¯ ∈ E(τ ) such that uτ (x1 (τ, ˆ e \ e¯(τ ), p(ˆ e \ e¯(τ )))) > 12

ˆ \ e¯(τ ), p(b ˆ \ e¯(τ )))) = uτ (x1 (τ, ˆ uτ (x1 (τ, ˆ e(τ ), p(ˆ e))). Then, uτ (x(τ, b e\ 1 10 ˆ ˆ e¯(τ ), p(ˆ e \ e¯(τ )))) > uτ (x (τ, ˆ e(τ ), p(ˆ e))) = uτ (x(τ, b(τ ), p(b))) as p (ˆ e\ ˆ \ e¯(τ )), a contradiction. Therefore, ut (x1 (t, ˆ e¯(τ )) = p(b e(t), p(ˆ e))) ≥ ut (x1 (t, ˆ e \e(t), p(ˆ e \e(t)))), for each e ∈ E(t) and for each t ∈ T1 . Hence, the ˆ ˆ = x1 (t, ˆ pair (ˆ e, x ˆ), where x ˆ(t) = x(t, b(t), p(b)) e(t), p10 (ˆ e)), for each t ∈ T1 , 0 10 ˆ ˆ and x ˆ(t) = x(t, b(t), p(b)) = x (t, p (ˆ e)), for each t ∈ T0 , is a CournotWalras equilibrium of E. (ii) Let (˜ e, x ˜) be a Cournot-Walras equilibrium of ˜ be a strategy selection such that b(t) ˜ E. Let b =˜ e10 (t), for each t ∈ T . 10 ¯ ¯ ¯ ˜ = p(˜ ˜ is irreducible and p(b) ˜ =E ˜ and p(˜ Then, B e) as B e) satisfies Equa˜ ˜ tion (4). But then, it is straightforward to verify that x ˜(t) = x(t, b(t), p(b)), for each t ∈ T . Suppose that there is a trader τ ∈ T1 and a strategy ¯b ∈ B(τ ) such that uτ (x(τ, b ˜ \ ¯b(τ ), p(b ˜ \ ¯b(τ )))) > uτ (x(τ, b(τ ˜ ), p(b))). ˜ 1 ¯ ¯ ¯ ¯ ˜ ˜ Then, uτ (x (τ, ˜ e \ b(τ ), p(˜ e \ b(τ )))) = uτ (x(τ, b \ b(τ ), p(b \ b(τ )))) > ˜ ), p(b))) ˜ ˜ \ ¯b(τ )) = p(˜ uτ (x(τ, b(τ = uτ (x1 (τ, ˜ e(τ ), p(˜ e))), as p(b e \ ¯b(τ )), ˜ ˜ ˜ ˜ a contradiction. Therefore, ut (x(t, b(t), p(b)) ≥ ut (x(t, b \ b(t), p(b \ b(t)))), ˜ ˜ ≥ for each b ∈ B(t) and for each t ∈ T1 . Moreover, ut (x(t, b(t), p(b)) ˜ \ b(t), p(b ˜ \ b(t)))), for each b ∈ B(t) and for each t ∈ T0 , by the ut (x(t, b ˜ is a Cobb-Douglassame argument used in the proof of Theorem 1. Hence, b Cournot-Nash equilibrium of Γ. The following corollary is a straightforward consequence of Theorem 2. Corollary. Under Assumptions 1, 2, and 3, there exists a Cournot-Walras equilibrium of E, (˜ e, x ˜).

6

Conclusion

In this paper, we reconsidered two models of noncooperative oligopoly in general equilibrium which are both a reformulation of a particular strategic market game, the so called Shapley’s window model, introduced by Busetto et al. (2008), (2011). The novelty introduced in this paper is the assumption that the preferences of the traders belonging to the atomless part are represented by Cobb-Douglas utility functions. Two kind of results are obtained. First, we proved the existence of a Cobb-Douglas-Cournot-Nash equilibrium. Second, we showed the equivalence between the set of the Cobb-DouglasCournot-Nash equilibrium allocations and the set of the Cournot-Walras equilibrium allocations. Busetto et al. (2012) have investigated the limit relationship between the Cournot-Nash and the Walras equilibrium. They partially replicated 13

the exchange economy by increasing the number of atoms without affecting the atomless part while ensuring that the measure space of agents remains finite. Then, they showed that any sequence of Cournot-Nash equilibrium allocations of the strategic market game associated with the partially replicated exchange economies approximates a Walras equilibrium allocation of the original exchange economy. A next step of our analysis could be to undertake a similar investigation in the framework of this paper.

References [1] Aliprantis C.D., Border K.C. (2006), Infinite dimensional analysis, Springer, New York. [2] Amir R., Sahi S., Shubik M., Yao S. (1990), “A strategic market game with complete markets,” Journal of Economic Theory 51, 126-143. [3] Busetto F., Codognato G., Ghosal S. (2008), “Cournot-Walras equilibrium as a subgame perfect equilibrium,” International Journal of Game Theory 37, 371-386. [4] Busetto F., Codognato G., Ghosal S. (2011), “Noncooperative oligopoly in markets with a continuum of traders,” Games and Economic Behavior, 72, 38-45. [5] Busetto F., Codognato G., Ghosal S. (2012), “Noncooperative oligopoly in markets with a continuum of traders: a limit theorem,” Working Paper n. 2012-49, EconomiX, Universit´e de Paris Ouest Nanterre la D´efense. [6] Codognato G., Gabszewicz J.J. (1993), “Cournot-Walras equilibria in markets with a continuum of traders,” Economic Theory 3, 453-464. [7] Codognato G., Ghosal S. (2000), “Cournot-Nash equilibria in limit exchange economies with complete markets and consistent prices,” Journal of Mathematical Economics 34, 39-53. [8] Cournot A. (1838), Recherches sur les principes math´ematiques de la th´eorie des richesses, Hachette, Paris. [9] d’Aspremont C., Dos Santos Ferreira R., G´erard-Varet L.-A. (1997), “General equilibrium concepts under imperfect competition: a Cournotian approach,” Journal of Economic Theory 73, 199-230. 14

[10] Dierker H., Grodal B. (1986), “Nonexistence of Cournot-Walras equilibrium in a general equilibrium model with two oligopolists,” in Hildenbrand W., Mas-Colell A. (eds), Contributions to mathematical economics in honor of G´erard Debreu, North-Holland, Amsterdam. [11] Dubey P., Shapley L.S. (1994), “Noncooperative general exchange with a continuum of traders: two models, ” Journal of Mathematical Economics 23, 253-293. [12] Dubey P., Shubik M. (1978), “The noncooperative equilibria of a closed trading economy with market supply and bidding strategies,” Journal of Economic Theory 17, 1-20. [13] Gabszewicz J.J., Michel P. (1997), “Oligopoly equilibrium in exchange economies,” in Eaton B.C., Harris R. G. (eds), Trade, technology and economics. Essays in honour of Richard G. Lipsey, Edward Elgar, Cheltenham. [14] Gabszewicz J.J., Vial J.-P. (1972), “Oligopoly ‘`a la Cournot-Walras’ in a general equilibrium analysis,” Journal of Economic Theory 4, 381-400. [15] Julien L.A., Tricou F. (2005), “Specialized oligopolies in a pure exchange economy: the symmetric Cournot-Walras equilibrium,” Research in Economics 59, 280-292. [16] Julien L.A., Tricou F. (2009), “Preferences, market power and oligopolistic competition: an example,” Economics Bulletin 29, 29182923. [17] Okuno M., Postlewaite A., Roberts J. (1980), “Oligopoly and competition in large markets,” American Economic Review 70, 22-31. [18] Mas-Colell A. (1982), “The Cournotian foundations of Walrasian equilibrium theory,” in Hildenbrand W. (ed), Advances in economic theory, Cambridge University Press, Cambridge. [19] Peck J., Shell K., Spear S.E. (1992), “The market game: existence and structure of equilibrium,” Journal of Mathematical Economics 21, 271-299. [20] Postlewaite A., Schmeidler D. (1978), “Approximate efficiency of nonWalrasian Nash equilibria,” Econometrica 46, 127-137. 15

[21] Roberts D.J., Sonnenschein H. (1977), “On the foundations of the theory of monopolistic competition,” Econometrica 45, 101-114. [22] Roberts K. (1980), “The limit points of monopolistic competition,” Journal of Economic Theory 22, 256-278. [23] Sahi S., Yao S. (1989), “The noncooperative equilibria of a trading economy with complete markets and consistent prices,” Journal of Mathematical Economics 18, 325-346. [24] Shapley L.S., Shubik M. (1977), “Trade using one commodity as a means of payment,” Journal of Political Economy 85, 937-968. [25] Shitovitz B. (1973), “Oligopoly in markets with a continuum of traders,” Econometrica 41, 467-501. [26] Shitovitz B. (1997), “A comparison between the core and the monopoly solutions in a mixed exchange economy,” Economic Theory 10, 559-563.

16

Noncooperative Oligopoly in Markets with a Cobb ...

solutions in theoretical models, Cobb-Douglas utility functions will turn out ..... an auxiliary game, which we call Γ1, where only the atoms act strategically,.

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