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Maladaptation and global indeterminacy

Published online by Cambridge University Press:  14 August 2019

Angelo Antoci
Affiliation:
Department of Economics and Business, University of Sassari, Sassari, Italy
Luca Gori*
Affiliation:
Department of Law, University of Pisa, Pisa, Italy
Mauro Sodini
Affiliation:
Department of Economics and Management, University of Pisa, Pisa, Italy
Elisa Ticci
Affiliation:
Department of Political and International Sciences, University of Siena, Siena, Italy
*
*Corresponding author. E-mail: luca.gori@unipi.it; dr.luca.gori@gmail.com
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Abstract

This article analyzes a general equilibrium growth model with overlapping generations and (production-induced) environmental degradation. Individuals react to environmental damages through mitigation or adaptation. In the former case, they reduce production and its environmental impact. In the latter, they do not tackle the causes of the problem but rather its consequences (i.e., the wellbeing loss due to environmental degradation) by increasing defensive expenditures. Despite its simplicity, the model can generate different long-term outcomes: convergence to a stationary state following a unique trajectory or local/global indeterminacy. In the last scenario, initial conditions (history) and individual expectations matter and the model can generate coordination failures and endogenous fluctuations. Results cast doubt on solutions to environmental problems relying on the role of individual behavior change or adaptation.

Information

Type
Research Article
Copyright
Copyright © Cambridge University Press 2019 
Figure 0

Figure 1. Determinacy/indeterminacy in the (β, δ)-plane. Parameter set: A = 10.6, α = 0.3, γ = 0.64 and θ = 0.2.

Figure 1

Figure 2. Local indeterminacy. Parameter set: A = 10.6, α = 0.3, γ = 0.64, θ = 0.2, δ = 0.14 and β = 1.1.

Figure 2

Figure 3. Values of $Q_{t}:=\sum_{n=0}^{t}U_{n}$ along the dashed and solid trajectories of figure 2. Parameter set: A = 10.6, α = 0.3, γ = 0.64, θ = 0.2, δ = 0.14 and β = 1.1.

Figure 3

Figure 4. Parameter set: A = 10.6, α = 0.3, $\beta = 0.89$, γ = 0.64, δ = 0.14 and θ = 0.2. Time series of two distinct trajectories of ℓt: one approaches the stationary state (dashed), which is saddle-point stable; the other approaches an attractive two-period cycle (solid).

Figure 4

Figure 5. (a) Bifurcation diagram for β. Parameter set: A = 0.3, α = 0.33, γ = 0.9, θ = 0.03 and δ = 0.4. (b) Bifurcation diagram for δ. Parameter set: A = 0.3, α = 0.33, γ = 0.9, θ = 0.03 and β = 0.28131. Multiple coexisting ω-limit sets.

Figure 5

Figure 6. Parameter set: A = 0.3, α = 0.33, γ = 0.9, θ = 0.03 and δ = 0.4. Time series of the variables K, ℓ and D showing the erratic behavior of a trajectory approaching the chaotic attractor, illustrated in the bifurcation diagram of figure 5, for β = 0.281310.