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Dynamic Government Performance: Honeymoons and Crises of Confidence

Published online by Cambridge University Press:  20 February 2012

TORUN DEWAN*
Affiliation:
London School of Economics and Political Science
DAVID P. MYATT*
Affiliation:
London Business School
*
Torun Dewan is Professor in Political Science, London School of Economics and Political Science, Houghton Street, London WC2A 2AEUnited Kingdom (t.dewan@lse.ac.uk).
David P. Myatt is Professor of Economics, London Business School, Regent's Park, London NW1 4SAUnited Kingdom (dmyatt@london.edu).
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Abstract

We use a formal theoretical framework to explore the interplay between a government's longevity and its performance. Ministers perform well when their careers are valuable; this is so when the government's duration is expected to be long; the government's survival depends on its popularity; and, finally, that popularity depends on its ministers’ performance. The feedback loop between performance and longevity means that multiple rational-expectations equilibria can arise: Ministers work hard for a popular government, but divert efforts elsewhere if they believe the government is doomed; these alternatives are both self-fulfilling prophecies. However, the presence of (perhaps small) random events that buffet the performance and popularity of a government is sufficient to pin down a unique equilibrium. We explore the dynamics that arise: A crisis of confidence involving the rapid collapse of a government's performance is sparked when a sequence of negative shocks push the popularity of the government below a unique critical threshold.

Information

Type
Research Article
Copyright
Copyright © American Political Science Association 2012
Figure 0

FIGURE 1.Government Effectiveness versus TenureNotes. Using data on 25 European democracies none of which have term limits, here we plot the World Bank Government Effectiveness Index (averaged over the years from 1996 to 2008) on the average length of government tenure during this period. Countries that have governments that survive longer on average also have more effective governments.

Figure 1

FIGURE 2.Prediction-market Confidence in the UK GovernmentNotes. These data from the intrade.com prediction market show the daily closing prices for a Labour victory in a UK General Election. (A contract pays 100 points if the specified event occurs.)

Figure 2

FIGURE 3.Declining Ministerial Performance with a Quadratic SpecificationNotes. This figure illustrates declining ministerial performance as the government's end nears. We use a quadratic linear specification: $u(e)=\bar{u} - \frac{e^2}{2}$ and $\lambda (e)=\bar{\lambda}-e$ where we assume that $\bar{\lambda}>\sqrt{2\bar{u}}$. We set V† = 0. For this specification, $e_t = V_t = \bar{\lambda}-\xi - \frac{2\xi (\bar{\lambda}-\xi)}{e^{\xi (T-t)}(\bar{\lambda}+\xi)-(\bar{\lambda}-\xi)}$ where $\xi \equiv \sqrt{\bar{\lambda}^2-2\bar{u}}$ and where the value of a career in an immortal government is $V^\ddag = \bar{\lambda}-\xi$.

Figure 3

FIGURE 4.Equilibrium Paths for PopularityNotes. This figure illustrates equilibrium paths for evolving popularity using the linear quadratic specification from Figure 3. The parameter choices are $\bar{\lambda}=1$, $\bar{u}=1.5$, and we specify r(e) = e−0.8. There are three equilibria, with three different lengths for the duration of the government. In the “good” equilibrium, optimism supports an immortal government (a terminal date of TH = ∞); popularity follows the solid line, rising until it hits the ceiling xH. In the “bad” equilibrium, pessimism corresponds to a short horizon TL; popularity follows the dashed line, falling monotonically. Finally, there is a non-monotonic equilibrium (the remaining broken line) in which the government lives until time TM. Popularity increases initially (but more slowly than in the optimistic equilibrium) until it reaches a maximum of x, and then it declines for the remaining τ periods of the government's life.

Figure 4

FIGURE 5.Markov Value Functions and the Popularity ThresholdNotes. This is value function V(x) for a Markovian equilibrium in a binary-action world. The lower bound for popularity is xL = 0; the terminal payoff for a minister is V† = 0. The other parameter choices are uL = 7, λL = 2, and rL = −1 for the low-performance regime; and uH = 4, λH = 1, and rH = 1 for the high-performance regime. Given that V† = 0, for the “pessimistic” regime where x < x*, the value function (the solid line in the figure) satisfies\protect\[V(x) = \frac{u_L}{\lambda _L}\left(1 - \exp \left[-\frac{\lambda _Lx}{|r_L|}\right] \right).\protect\]This function hits V* at a popularity level of x, which in this case satisfies x = log(7)/2; there is a Markovian equilibrium for any x* below this.

Figure 5

FIGURE 6.Value Function and Popularity Threshold with Random EventsNotes. This figure illustrates the value function V(x) and critical popularity threshold arising from the unique equilibrium of a binary-action world with randomly evolving popularity. The parameter choices (xL = 0, xH = 1.5, V† = 0, uL = 7, λL = 2,rL = −1, uH = 4, λH = 1, and rH = 1) match those used in Figure 5. The value function is plotted for three different choices of σ. The bullet points “●” indicate the location of the threshold x⋄ for these three cases. As σ → 0 the value function converges to the value function in Figure 5.

Figure 6

FIGURE 7.Sample Path of Evolving PopularityNotes. This is a sample path for evolving popularity, generated using a discrete-time approximation to our continuous-time specification. The parameter choices (xL = 0, xH = 1.5, V† = 0, uL = 7, λL = 2,rL = −1, uH = 4, λH = 1, and rH = 1), which match those used in Figures 5 and 6, are supplemented with a variance of σ2 = 0.5. This generates an equilibrium threshold satisfying x*≈0.875. The discrete-time approximation uses a time step of Δt = 0.005.

Figure 7

FIGURE 8.Equilibrium Popularity Paths in the Day-of-Reckoning ModelNotes. This figure illustrates possible equilibrium paths for popularity. The upper broken line is xt (see Proposition 5). Above it, the government always survives reelection; the top solid arrow shows such an equilibrium path, beginning from the “○” symbol. The lower broken line is $\underline{x}_t$ (see again Proposition 5). Below, the government is always defeated; again, a solid arrow shows the equilibrium path. Between the two broken lines, there are both “good” and “bad” equilibria. For instance, starting from the remaining “○” symbol there is a unique equilibrium path with growing popularity until time $t=T-\bar{\tau}$. However, for $t>T-\bar{\tau}$ there are two possibilities: popularity continues to grow in an optimistic equilibrium, ending above x† and so justifying the optimism; or, popularity falls in a pessimistic equilibrium, ends below x†, and the government falls.

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