equilibrium and stability in economic dynamics · · 2012-02-21international workshop on economic...
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Equilibrium and Stability in EconomicDynamics
Alfredo Medio
Department of Statistics, University of Udine
International Workshop on Economic Dynamics,University of Siena, Collegio S. Chiara
18-19 December 2009
Alfredo Medio Equilibrium and Stability
Disequilibrium Dynamics
John Chipman (1965), economist
The real content of the equilibrium concept is to befound not so much in the state itself as in the laws ofchange which it implies; that is in the tendencies tomove towards it, away from it, or around it
Brian Skyrms (1992), philosopher, game theorist
The explanatory value of equilibrium depends onthe underlying dynamics. When the underlyingdynamics is taken seriously, it becomes apparent thatequilibrium is not the central explanatory concept
Alfredo Medio Equilibrium and Stability
Canonical Dynamical Systems
1 Discrete Timext+1 = G(xt ;α) (1)
x ∈ Rn: state variables
G : U → Rm: “law of motion”
α ∈ Rm: given parameters
t ∈ Z+: time
2 Continuous Time
x = f (x ;α) (2)
x ≡ d/dtf : U → R
m
t ∈ R
Alfredo Medio Equilibrium and Stability
Canonical Dynamical Systems
1 Discrete Timext+1 = G(xt ;α) (1)
x ∈ Rn: state variables
G : U → Rm: “law of motion”
α ∈ Rm: given parameters
t ∈ Z+: time
2 Continuous Time
x = f (x ;α) (2)
x ≡ d/dtf : U → R
m
t ∈ R
Alfredo Medio Equilibrium and Stability
Definition
An orbit is a time–ordered collection of states of a dynamicalsystem starting from a given initial point. In continuous time, anorbit defines a curve {x(t)|t ∈ I ⊂ R}, in discrete–time it is asequence of discrete points (x0, G(x0), G2(x0), . . .)
Definition
equilibrium is a fixed point x of (1) or (2), such that G(x) = x(discrete case) , or f (x) = 0 (continuous case)
Definition
A set A ⊂ Rn is invariant if orbits never leave it under the action
of G (or f )
Alfredo Medio Equilibrium and Stability
Definition
An orbit is a time–ordered collection of states of a dynamicalsystem starting from a given initial point. In continuous time, anorbit defines a curve {x(t)|t ∈ I ⊂ R}, in discrete–time it is asequence of discrete points (x0, G(x0), G2(x0), . . .)
Definition
equilibrium is a fixed point x of (1) or (2), such that G(x) = x(discrete case) , or f (x) = 0 (continuous case)
Definition
A set A ⊂ Rn is invariant if orbits never leave it under the action
of G (or f )
Alfredo Medio Equilibrium and Stability
Definition
An orbit is a time–ordered collection of states of a dynamicalsystem starting from a given initial point. In continuous time, anorbit defines a curve {x(t)|t ∈ I ⊂ R}, in discrete–time it is asequence of discrete points (x0, G(x0), G2(x0), . . .)
Definition
equilibrium is a fixed point x of (1) or (2), such that G(x) = x(discrete case) , or f (x) = 0 (continuous case)
Definition
A set A ⊂ Rn is invariant if orbits never leave it under the action
of G (or f )
Alfredo Medio Equilibrium and Stability
Stability: there are more than 50 definitions of stability,but...
Definition
A point, or a set, is weakly (Lyapunov) stable if orbits startingnear it stay near
Definition
A point, or a set, is strongly (asymptotically) stable if (i) it isweakly stable and (ii) orbits starting in a (not too small) basinconverge to it
Alfredo Medio Equilibrium and Stability
Stability: there are more than 50 definitions of stability,but...
Definition
A point, or a set, is weakly (Lyapunov) stable if orbits startingnear it stay near
Definition
A point, or a set, is strongly (asymptotically) stable if (i) it isweakly stable and (ii) orbits starting in a (not too small) basinconverge to it
Alfredo Medio Equilibrium and Stability
Strategy
locate equilibria (invariant sets) and investigate theirstability properties
study the behavior of typical orbits (in a topological ormetric sense)
study effects of changing parameters (bifurcation theory)
Alfredo Medio Equilibrium and Stability
Strategy
locate equilibria (invariant sets) and investigate theirstability properties
study the behavior of typical orbits (in a topological ormetric sense)
study effects of changing parameters (bifurcation theory)
Alfredo Medio Equilibrium and Stability
Strategy
locate equilibria (invariant sets) and investigate theirstability properties
study the behavior of typical orbits (in a topological ormetric sense)
study effects of changing parameters (bifurcation theory)
Alfredo Medio Equilibrium and Stability
Models of Disequilibrium Dynamics
Example
Multiplier–accelerator cycle models: e.g., Samuelson (1939),Kaldor (1940), Hicks (1950), Goodwin (1951), Kalecki (1954)
aggregate “stylized facts”, instead of “first principles”
lags and nonlinearities
adaptive, backward–looking adjusting mechanism
methods: stability analysis, phase–diagrams,Poincaré–Bendixson Theorem
result: conditions for persistent oscillations
Alfredo Medio Equilibrium and Stability
Models of Disequilibrium Dynamics
Example
Multiplier–accelerator cycle models: e.g., Samuelson (1939),Kaldor (1940), Hicks (1950), Goodwin (1951), Kalecki (1954)
aggregate “stylized facts”, instead of “first principles”
lags and nonlinearities
adaptive, backward–looking adjusting mechanism
methods: stability analysis, phase–diagrams,Poincaré–Bendixson Theorem
result: conditions for persistent oscillations
Alfredo Medio Equilibrium and Stability
Models of Disequilibrium Dynamics
Example
Multiplier–accelerator cycle models: e.g., Samuelson (1939),Kaldor (1940), Hicks (1950), Goodwin (1951), Kalecki (1954)
aggregate “stylized facts”, instead of “first principles”
lags and nonlinearities
adaptive, backward–looking adjusting mechanism
methods: stability analysis, phase–diagrams,Poincaré–Bendixson Theorem
result: conditions for persistent oscillations
Alfredo Medio Equilibrium and Stability
Models of Disequilibrium Dynamics
Example
Multiplier–accelerator cycle models: e.g., Samuelson (1939),Kaldor (1940), Hicks (1950), Goodwin (1951), Kalecki (1954)
aggregate “stylized facts”, instead of “first principles”
lags and nonlinearities
adaptive, backward–looking adjusting mechanism
methods: stability analysis, phase–diagrams,Poincaré–Bendixson Theorem
result: conditions for persistent oscillations
Alfredo Medio Equilibrium and Stability
Models of Disequilibrium Dynamics
Example
Multiplier–accelerator cycle models: e.g., Samuelson (1939),Kaldor (1940), Hicks (1950), Goodwin (1951), Kalecki (1954)
aggregate “stylized facts”, instead of “first principles”
lags and nonlinearities
adaptive, backward–looking adjusting mechanism
methods: stability analysis, phase–diagrams,Poincaré–Bendixson Theorem
result: conditions for persistent oscillations
Alfredo Medio Equilibrium and Stability
Example
Tâtonnement: Walras (1926 [1874]), ..., Arrow and Hurwicz(1958) and Arrow, Block and Hurwicz(1959)
rational (mazimizing) agents; macroeconomic compatibility(markets clear); no “false trading”
adjustment: “law of demand and supply”
method: second method of Lyapunov
result: equilibrium strongly stable only under stringentassumptions (gross substitutability)
Alfredo Medio Equilibrium and Stability
Example
Tâtonnement: Walras (1926 [1874]), ..., Arrow and Hurwicz(1958) and Arrow, Block and Hurwicz(1959)
rational (mazimizing) agents; macroeconomic compatibility(markets clear); no “false trading”
adjustment: “law of demand and supply”
method: second method of Lyapunov
result: equilibrium strongly stable only under stringentassumptions (gross substitutability)
Alfredo Medio Equilibrium and Stability
Example
Tâtonnement: Walras (1926 [1874]), ..., Arrow and Hurwicz(1958) and Arrow, Block and Hurwicz(1959)
rational (mazimizing) agents; macroeconomic compatibility(markets clear); no “false trading”
adjustment: “law of demand and supply”
method: second method of Lyapunov
result: equilibrium strongly stable only under stringentassumptions (gross substitutability)
Alfredo Medio Equilibrium and Stability
Example
Tâtonnement: Walras (1926 [1874]), ..., Arrow and Hurwicz(1958) and Arrow, Block and Hurwicz(1959)
rational (mazimizing) agents; macroeconomic compatibility(markets clear); no “false trading”
adjustment: “law of demand and supply”
method: second method of Lyapunov
result: equilibrium strongly stable only under stringentassumptions (gross substitutability)
Alfredo Medio Equilibrium and Stability
Example
Tâtonnement: Walras (1926 [1874]), ..., Arrow and Hurwicz(1958) and Arrow, Block and Hurwicz(1959)
rational (mazimizing) agents; macroeconomic compatibility(markets clear); no “false trading”
adjustment: “law of demand and supply”
method: second method of Lyapunov
result: equilibrium strongly stable only under stringentassumptions (gross substitutability)
Alfredo Medio Equilibrium and Stability
Example
Tâtonnement: Walras (1926 [1874]), ..., Arrow and Hurwicz(1958) and Arrow, Block and Hurwicz(1959)
rational (mazimizing) agents; macroeconomic compatibility(markets clear); no “false trading”
adjustment: “law of demand and supply”
method: second method of Lyapunov
result: equilibrium strongly stable only under stringentassumptions (gross substitutability)
Alfredo Medio Equilibrium and Stability
The Abandonment of Disequilibrium Dynamics
Muth (1961), Hahn (1974), Prescott and Mehra (1980), Lucas(1996, Nobel Lecture)
the scientist’s approach (as in Chipman’s and Skyrms’squotes) is rejected: equilibrium is the central explanatoryconcept of economic analysis
rational expectations: only non–systematic mistakes areallowed; probability distributions on which agents’decisions are based are the same as those resulting fromthose decisions (in a deterministic context, this amounts to“perfect foresight”)
Alfredo Medio Equilibrium and Stability
The Abandonment of Disequilibrium Dynamics
Muth (1961), Hahn (1974), Prescott and Mehra (1980), Lucas(1996, Nobel Lecture)
the scientist’s approach (as in Chipman’s and Skyrms’squotes) is rejected: equilibrium is the central explanatoryconcept of economic analysis
rational expectations: only non–systematic mistakes areallowed; probability distributions on which agents’decisions are based are the same as those resulting fromthose decisions (in a deterministic context, this amounts to“perfect foresight”)
Alfredo Medio Equilibrium and Stability
Recursive Equilibrium Dynamics
Dynamics are not generated by off–equilibrium forces butare derived from equilibrium conditions
Agents’ maximizing behavior + clearing markets +intertemporal constraints generate the implicit “law ofmotion”, with or without uncertainty
disequilibrium analysis is disqualified becausedisequilibrium behavior is irrational and therefore is not a“proper economic behavior”
Alfredo Medio Equilibrium and Stability
Recursive Equilibrium Dynamics
Dynamics are not generated by off–equilibrium forces butare derived from equilibrium conditions
Agents’ maximizing behavior + clearing markets +intertemporal constraints generate the implicit “law ofmotion”, with or without uncertainty
disequilibrium analysis is disqualified becausedisequilibrium behavior is irrational and therefore is not a“proper economic behavior”
Alfredo Medio Equilibrium and Stability
Recursive Equilibrium Dynamics
Dynamics are not generated by off–equilibrium forces butare derived from equilibrium conditions
Agents’ maximizing behavior + clearing markets +intertemporal constraints generate the implicit “law ofmotion”, with or without uncertainty
disequilibrium analysis is disqualified becausedisequilibrium behavior is irrational and therefore is not a“proper economic behavior”
Alfredo Medio Equilibrium and Stability
Example
I. Optimal growth
Ramsey problem, discrete time
solution orbits correspond to equilibria of the completemarket, Arrow–Debreu model
application of Bellman’s dynamic programming equationand the associate policy function may reduce the problemto a recursive model (in appropriate state variables)
result: “anything goes”; equilibrium orbits may tend to astationary equilibrium, to periodic or even chaotic sets
Alfredo Medio Equilibrium and Stability
Example
I. Optimal growth
Ramsey problem, discrete time
solution orbits correspond to equilibria of the completemarket, Arrow–Debreu model
application of Bellman’s dynamic programming equationand the associate policy function may reduce the problemto a recursive model (in appropriate state variables)
result: “anything goes”; equilibrium orbits may tend to astationary equilibrium, to periodic or even chaotic sets
Alfredo Medio Equilibrium and Stability
Example
I. Optimal growth
Ramsey problem, discrete time
solution orbits correspond to equilibria of the completemarket, Arrow–Debreu model
application of Bellman’s dynamic programming equationand the associate policy function may reduce the problemto a recursive model (in appropriate state variables)
result: “anything goes”; equilibrium orbits may tend to astationary equilibrium, to periodic or even chaotic sets
Alfredo Medio Equilibrium and Stability
Example
I. Optimal growth
Ramsey problem, discrete time
solution orbits correspond to equilibria of the completemarket, Arrow–Debreu model
application of Bellman’s dynamic programming equationand the associate policy function may reduce the problemto a recursive model (in appropriate state variables)
result: “anything goes”; equilibrium orbits may tend to astationary equilibrium, to periodic or even chaotic sets
Alfredo Medio Equilibrium and Stability
Example
II. Overlapping generations models
no complete markets and unrestricted participation; doubleinfinity of agents and commodities
implicit dynamics:
F (xt , xt+1) = 0 (3)
if F can be inverted w.r.t. xt+1, (3) → (1)
result: “anything goes” againproblems (Medio and Raines, 2007):
backward dynamics, ifF can only be inverted w.r.t. xt
initial conditions (are they arbitrary?)
Alfredo Medio Equilibrium and Stability
Example
II. Overlapping generations models
no complete markets and unrestricted participation; doubleinfinity of agents and commodities
implicit dynamics:
F (xt , xt+1) = 0 (3)
if F can be inverted w.r.t. xt+1, (3) → (1)
result: “anything goes” againproblems (Medio and Raines, 2007):
backward dynamics, ifF can only be inverted w.r.t. xt
initial conditions (are they arbitrary?)
Alfredo Medio Equilibrium and Stability
Example
II. Overlapping generations models
no complete markets and unrestricted participation; doubleinfinity of agents and commodities
implicit dynamics:
F (xt , xt+1) = 0 (3)
if F can be inverted w.r.t. xt+1, (3) → (1)
result: “anything goes” againproblems (Medio and Raines, 2007):
backward dynamics, ifF can only be inverted w.r.t. xt
initial conditions (are they arbitrary?)
Alfredo Medio Equilibrium and Stability
Example
II. Overlapping generations models
no complete markets and unrestricted participation; doubleinfinity of agents and commodities
implicit dynamics:
F (xt , xt+1) = 0 (3)
if F can be inverted w.r.t. xt+1, (3) → (1)
result: “anything goes” againproblems (Medio and Raines, 2007):
backward dynamics, ifF can only be inverted w.r.t. xt
initial conditions (are they arbitrary?)
Alfredo Medio Equilibrium and Stability
Example
II. Overlapping generations models
no complete markets and unrestricted participation; doubleinfinity of agents and commodities
implicit dynamics:
F (xt , xt+1) = 0 (3)
if F can be inverted w.r.t. xt+1, (3) → (1)
result: “anything goes” againproblems (Medio and Raines, 2007):
backward dynamics, ifF can only be inverted w.r.t. xt
initial conditions (are they arbitrary?)
Alfredo Medio Equilibrium and Stability
Bounded Rationality
the perfect foresight/rational expectations hypothesisrequires some very demanding assumptions (e.g., a greatdeal of common knowledge, infinite and non–distortedmemory, a super–human calculating ability)
loosening one or the other of them yields non–equilibriumdynamics models, often in the form of iterated maps (withor without random elements)
Alfredo Medio Equilibrium and Stability
Bounded Rationality
the perfect foresight/rational expectations hypothesisrequires some very demanding assumptions (e.g., a greatdeal of common knowledge, infinite and non–distortedmemory, a super–human calculating ability)
loosening one or the other of them yields non–equilibriumdynamics models, often in the form of iterated maps (withor without random elements)
Alfredo Medio Equilibrium and Stability
Bounded Rationality
the perfect foresight/rational expectations hypothesisrequires some very demanding assumptions (e.g., a greatdeal of common knowledge, infinite and non–distortedmemory, a super–human calculating ability)
loosening one or the other of them yields non–equilibriumdynamics models, often in the form of iterated maps (withor without random elements)
Alfredo Medio Equilibrium and Stability
Example
forecasting methods (homogeneous or heterogeneous,e.g. Brock and Hommes (1997))
learning (“eductive”, trial–and–error, etc., e.g. Binmore(1990), Gale (2000))
dynamic games (fictitious games, evolutionary games, e.g.Skyrms (1992))
Alfredo Medio Equilibrium and Stability
Random Difference Equations
Recursive equilibrium, or bounded rationality models +random perturbations with a Markov representation
two basic types: perturbations of fundamentals (tastes andtechnology) and perturbations of expectations (sunspots)
Basic Stochastic Equations
xt+1 = T (xt , εξt+1)
xt+1 = T (xt , εξt+1) = F (xt)︸ ︷︷ ︸
deterministic core
+ G(xt , εξt+1)︸ ︷︷ ︸
perturbation term
F (xt) = T (xt , 0) ∀t ≥ 0G(xt , 0) = 0 ∀x
Alfredo Medio Equilibrium and Stability
Random Difference Equations
Recursive equilibrium, or bounded rationality models +random perturbations with a Markov representation
two basic types: perturbations of fundamentals (tastes andtechnology) and perturbations of expectations (sunspots)
Basic Stochastic Equations
xt+1 = T (xt , εξt+1)
xt+1 = T (xt , εξt+1) = F (xt)︸ ︷︷ ︸
deterministic core
+ G(xt , εξt+1)︸ ︷︷ ︸
perturbation term
F (xt) = T (xt , 0) ∀t ≥ 0G(xt , 0) = 0 ∀x
Alfredo Medio Equilibrium and Stability
Random Difference Equations
Recursive equilibrium, or bounded rationality models +random perturbations with a Markov representation
two basic types: perturbations of fundamentals (tastes andtechnology) and perturbations of expectations (sunspots)
Basic Stochastic Equations
xt+1 = T (xt , εξt+1)
xt+1 = T (xt , εξt+1) = F (xt)︸ ︷︷ ︸
deterministic core
+ G(xt , εξt+1)︸ ︷︷ ︸
perturbation term
F (xt) = T (xt , 0) ∀t ≥ 0G(xt , 0) = 0 ∀x
Alfredo Medio Equilibrium and Stability
Random Difference Equations
Recursive equilibrium, or bounded rationality models +random perturbations with a Markov representation
two basic types: perturbations of fundamentals (tastes andtechnology) and perturbations of expectations (sunspots)
Basic Stochastic Equations
xt+1 = T (xt , εξt+1)
xt+1 = T (xt , εξt+1) = F (xt)︸ ︷︷ ︸
deterministic core
+ G(xt , εξt+1)︸ ︷︷ ︸
perturbation term
F (xt) = T (xt , 0) ∀t ≥ 0G(xt , 0) = 0 ∀x
Alfredo Medio Equilibrium and Stability
Dynamics of Probability Distributions
Transition Probability Kernel
Pε(x , A) =
∫
Wε
χA[T (x , εξ)]νε(dεξ) x ∈ X , A ∈ B(X )
πt+1(A) = P[πt (A)], π ∈ M
P[π(A)] =
∫
XP(x , A)π(dx)
π(A) =∫
P(x , A)π(dx) : invariant probability distribution
Alfredo Medio Equilibrium and Stability
Dynamics of Probability Distributions
Transition Probability Kernel
Pε(x , A) =
∫
Wε
χA[T (x , εξ)]νε(dεξ) x ∈ X , A ∈ B(X )
πt+1(A) = P[πt (A)], π ∈ M
P[π(A)] =
∫
XP(x , A)π(dx)
π(A) =∫
P(x , A)π(dx) : invariant probability distribution
Alfredo Medio Equilibrium and Stability
Dynamics of Probability Distributions
Transition Probability Kernel
Pε(x , A) =
∫
Wε
χA[T (x , εξ)]νε(dεξ) x ∈ X , A ∈ B(X )
πt+1(A) = P[πt (A)], π ∈ M
P[π(A)] =
∫
XP(x , A)π(dx)
π(A) =∫
P(x , A)π(dx) : invariant probability distribution
Alfredo Medio Equilibrium and Stability
Stochastic Stability
A general result on stochastic stability, Medio (2004)
1 applications: perturbed optimal growth models; sunspotOLG models (with well–defined forward dynamics);(bounded rationality) models of dynamic matching andbargaining games, with a Markov representation
2 state variables and random variables take values ingeneral space
3 result applies to any type of deterministic attracting set Λ(fixed point, periodic, chaotic)
Alfredo Medio Equilibrium and Stability
Stochastic Stability
A general result on stochastic stability, Medio (2004)
1 applications: perturbed optimal growth models; sunspotOLG models (with well–defined forward dynamics);(bounded rationality) models of dynamic matching andbargaining games, with a Markov representation
2 state variables and random variables take values ingeneral space
3 result applies to any type of deterministic attracting set Λ(fixed point, periodic, chaotic)
Alfredo Medio Equilibrium and Stability
Stochastic Stability
A general result on stochastic stability, Medio (2004)
1 applications: perturbed optimal growth models; sunspotOLG models (with well–defined forward dynamics);(bounded rationality) models of dynamic matching andbargaining games, with a Markov representation
2 state variables and random variables take values ingeneral space
3 result applies to any type of deterministic attracting set Λ(fixed point, periodic, chaotic)
Alfredo Medio Equilibrium and Stability
Assumptions
1 regularity of maps and perturbations2 the deterministic map F possesses an asymptotically
stable attracting set Λ with basin B(Λ)
3 the perturbation is sufficiently small (ε small) w.r.t. the sizeof B(Λ) and the strength of attraction
Alfredo Medio Equilibrium and Stability
Assumptions
1 regularity of maps and perturbations2 the deterministic map F possesses an asymptotically
stable attracting set Λ with basin B(Λ)
3 the perturbation is sufficiently small (ε small) w.r.t. the sizeof B(Λ) and the strength of attraction
Alfredo Medio Equilibrium and Stability
Assumptions
1 regularity of maps and perturbations2 the deterministic map F possesses an asymptotically
stable attracting set Λ with basin B(Λ)
3 the perturbation is sufficiently small (ε small) w.r.t. the sizeof B(Λ) and the strength of attraction
Alfredo Medio Equilibrium and Stability
Transitivity (indecomposability)
Three cases:1 Case 1. Λ is strongly indecomposable (F strongly
topologically transitive) (e.g. Λ is a fixed point or a mixingchaotic set)
2 Case 2. F is topologically transitive on Λ but not stronglyso (e.g., Λ is a periodic set or a non–mixing chaotic set)
3 Case 3. F is not topologically transitive on Λ (e.g., thereexist multiple attractors for the map F )
Alfredo Medio Equilibrium and Stability
Transitivity (indecomposability)
Three cases:1 Case 1. Λ is strongly indecomposable (F strongly
topologically transitive) (e.g. Λ is a fixed point or a mixingchaotic set)
2 Case 2. F is topologically transitive on Λ but not stronglyso (e.g., Λ is a periodic set or a non–mixing chaotic set)
3 Case 3. F is not topologically transitive on Λ (e.g., thereexist multiple attractors for the map F )
Alfredo Medio Equilibrium and Stability
Transitivity (indecomposability)
Three cases:1 Case 1. Λ is strongly indecomposable (F strongly
topologically transitive) (e.g. Λ is a fixed point or a mixingchaotic set)
2 Case 2. F is topologically transitive on Λ but not stronglyso (e.g., Λ is a periodic set or a non–mixing chaotic set)
3 Case 3. F is not topologically transitive on Λ (e.g., thereexist multiple attractors for the map F )
Alfredo Medio Equilibrium and Stability
Stochastic Stability
1 Case 1: for each ε the operator P convergesasymptotically to a unique, invariant distribution πε
2 Case 2: there exist a finite number d of invariant (possiblyidentical) distributions. The operator (P)d converges to aunique distribution depending on the initial conditions
3 Case 3: there exists a finite decomposition of the statespace X into absorbing sets. If we restrict the dynamics ofT to one or the other of these sets, we are back to case 1or 2
Alfredo Medio Equilibrium and Stability
Stochastic Stability
1 Case 1: for each ε the operator P convergesasymptotically to a unique, invariant distribution πε
2 Case 2: there exist a finite number d of invariant (possiblyidentical) distributions. The operator (P)d converges to aunique distribution depending on the initial conditions
3 Case 3: there exists a finite decomposition of the statespace X into absorbing sets. If we restrict the dynamics ofT to one or the other of these sets, we are back to case 1or 2
Alfredo Medio Equilibrium and Stability
Stochastic Stability
1 Case 1: for each ε the operator P convergesasymptotically to a unique, invariant distribution πε
2 Case 2: there exist a finite number d of invariant (possiblyidentical) distributions. The operator (P)d converges to aunique distribution depending on the initial conditions
3 Case 3: there exists a finite decomposition of the statespace X into absorbing sets. If we restrict the dynamics ofT to one or the other of these sets, we are back to case 1or 2
Alfredo Medio Equilibrium and Stability
A bouquet of simple ideas
1 in the theory of competitive general equilibrium anormative notion of equilibrium prevails
2 in a descriptive sense, equilibrium loses much of itsplausibility without an account of the dynamics that bring itabout
3 mathematical stability theory retains a fundamentalimportance in the economist’s toolkit
4 in the presence of random perturbations, the dynamics of asystem are best described in terms of probabilitydistributions and their stochastic stability. This significantlyblurs the differences among the canonical types ofattractors (fixed points, periodic and chaotic sets)
Alfredo Medio Equilibrium and Stability
References I
Arrow, K. J. and L. Hurwicz, 1958. On the stability of thecompetitive equilibrium I,Econometrica, 26, 522–52
Arrow, K. J., H. D. Block and L. Hurwicz, 1959. On the stabilityof the competitive equilibrium II,Econometrica27, 82–109
Binmore, K. 1990. Modelling Rational Players: Parts I and II, in:K. Binmore,Essays on the Foundations of Game Theory, Oxfordand Cambbridge, MA: Blackwell, 151–185, 186–231
Brock, W.A. and C.H. Hommes, 1997. A Rational Route toRandomness,Econometrica, 65(5), 1059-1096,
Chipman, John S. 1965. The Nature and Meaning of Equilibriumin Economic Theory, in: H. Townsend (ed.),Price Theory,Middlesex, England: Penguin Books, 341–372
Gale, D. 2000.Strategic Foundations of General Equilibrium,Cambridge: Cambridge University Press
Alfredo Medio Equilibrium and Stability
References II
Goodwin, R.M., 1951. The nonlinear accelerator and thepersistence of business cycles.Econometrica, 19, 1–17.
Hahn, F. 1974. On the Notion of Equilibrium in Economics,Inaugural Lecture, Cambridge University, reprinted in F. Hahn,Equilibrium and Macroeconomics, Cambridge MA.: MIT Press,1984
Hicks, J. A., 1950.Contribution to the Theory of the Trade CycleOxford: Clarendon Press
Kaldor, N., 1940. A model of the trade cycle.Economic Journal,50, 78–92
Kalecki, M., 1954.Theory of economic dynamics: An essay oncyclical and long- run changes in capitalist economy, London:Allen and Unwin
Alfredo Medio Equilibrium and Stability
References III
Medio, A. 2004. Invariant Probabaility Distributions inEconomic Models: A General Result,MacroeconomicDynamics, 8, 162–187
Medio, A. and B. Raines, 2007. Backward Dynamics inEconomics. The Inverse Limit Approach,Journal of EconomicDynamics and Control, 31 1633-1671
Muth, J., 1961. Rational expectations and the theory of pricemovements.Econometrica, 29, 315–335
Prescott, E.C. and R. Mehra, 1980. Recursive CompetitiveEquilibrium: The Case of Homogeneous Households,Econometrica48, No. 6, 1365–1379
Lucas, R.E., Jr. 1996. Nobel Lecture: Monetary Neutrality,TheJournal of Political Economy, 104, No. 4, 661–682
Alfredo Medio Equilibrium and Stability
References IV
Samuelson, P. A., 1939. Interaction Between the MultiplierAnalysis and the Principle of Acceleration,Review of EconomicStatistics21, 75–78
Skyrms, B. 1992. Chaos and the Explanatory Significance ofEquilibrium: Strange Attractors in Evolutionary GameDynamics,PSA, Volume 2 374-394
Walras, L., 1926.Élements d’économie politique pure; ou,Théorie de la richesse sociale. Paris: Pichon et Durand-Auzias;Lausanne: Rouge
Alfredo Medio Equilibrium and Stability