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The Autocrat's Credibility Problem and Foundations of the Constitutional State

Published online by Cambridge University Press:  01 February 2008

ROGER B. MYERSON*
Affiliation:
University of Chicago
*
Roger B. Myerson is Professor, Department of Economics, University of Chicago, 1126 East 59th Street, Chicago, IL 60637 (myerson@uchicago.edu).
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Abstract

A political leader's temptation to deny costly debts to past supporters is a central moral-hazard problem in politics. This paper develops a game-theoretic model to probe the consequences of this moral-hazard problem for leaders who compete to establish political regimes. In contests for power, absolute leaders who are not subject to third-party judgments can credibly recruit only limited support. A leader can do better by organizing supporters into a court which could cause his downfall. In global negotiation-proof equilibria, leaders cannot recruit any supporters without such constitutional checks. Egalitarian norms make recruiting costlier in oligarchies, which become weaker than monarchies. The ruler's power and limitations on entry of new leaders are derived from focal-point effects in games with multiple equilibria. The relationships of trust between leaders and their supporters are personal constitutions which underlie all other political constitutions.

Information

Type
Research Article
Copyright
Copyright © American Political Science Association 2008
Figure 0

FIGURE 1.Optimal Sizes of Supporting Forces for Different Kinds of Regimes, Depending on the Anticipated Rival Forces, for Example, with R = 90, δ = 0.05, λ = 0.2, c = 5, and s = 1.5

Figure 1

FIGURE 2.Results of Changing the Size of the Supporting Force, Against m = 30, with R = 90, δ = 0.05, λ = 0.2, c = 5, and s = 1.5

Figure 2

FIGURE 3.Changes in Equilibrium for Different Values of λ, the Expected Rate of Challenges, with R = 90, δ = 0.05, c = 5, and s = 1.5

Figure 3

FIGURE 4.Discrete (Integer) Approximation of the Randomized Negotiation-Proof Equilibrium, for Example, with R = 90, δ = 0.05, λ = 0.2, c = 5, and s = 3

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