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Effects of Law-Enforcement Efficiency and Duration of Trials in an Oligopolistic Competition Among Fair and Unfair Firms

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Abstract

Building on differential game theory involving asymmetric agents, an oligopoly game between two distinct groups of firms is analyzed and solved under open-loop information. One group develops Research & Development to reduce its marginal production costs and behaves fairly, whereas the other one violates intellectual property rights of the rival, using the stolen technology to reduce its own marginal costs. We investigate the effects of law enforcement in this setup, by discussing the appropriate fine to be determined and the profitability of unfair behavior. Finally, we assess how the duration of related trials can affect efficiency of enforcement policy.

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Fig. 1
Fig. 2

Notes

  1. Clearly, a static game would fail to model the technological spillover effects and all the other circumstances evolving over time.

  2. Basically, we just take into account two types of firms. A further investigation on an oligopoly, where firms can switch from a type to another under some incentive scheme, whereby the sizes of the populations change over time, goes beyond the scope of this paper.

  3. This procedure is based on symmetry, meaning that this simplification basically leads to a duopoly with one fair and one unfair firm, which is the simplest circumstance, coinciding with the case where \(h=1\) and \(N=2\).

  4. This suggests a further interpretation for \(\epsilon \) as a constant, measuring the intensity of the reduction in the necessary Research & Development effort of the unique unfair firm, when the population of fair firms is very large.

  5. The complete calculations are available upon request to the authors.

  6. Alternatively, also the net value might be considered, that is, the discounted flow of profits, which includes production costs.

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Acknowledgments

This paper is part of the research project ’Culture, Justice and Growth’ funded by the Faculty of Economics of Sapienza University of Rome (2012). The authors thank Luca Lambertini, Cecilia Vergari, the audience in Oligo Workshop 2014 at Sapienza University of Rome and the three anonymous referees for valuable comments and suggestions, which were absolutely helpful to improve the paper. The usual disclaimer applies.

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Correspondence to Arsen Palestini.

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Communicated by Jean-Pierre Crouzeix.

Appendix

Appendix

Proof of Proposition 3.2

First, we state necessary conditions for open-loop equilibrium before imposing symmetry. By Pontryagin’s maximum principle, the costate equations of the model are:

$$\begin{aligned} \dot{\lambda }_{ii}(t)= & {} \rho \lambda _{ii}(t)-\dfrac{\partial \widetilde{H}_i}{\partial c_i}\nonumber \\ \Longrightarrow \ \dot{\lambda }_{ii}(t)= & {} (\rho -\delta ) \lambda _{ii}(t)+\dfrac{-(N-h+1)\widetilde{c}(t)+(N-h)\overline{c}(t)+A}{N+1}, \ i=1, \ldots , h, \nonumber \\ \end{aligned}$$
(29)
$$\begin{aligned} \dot{\lambda }_{ij}(t)= & {} \rho \lambda _{ij}(t)-\dfrac{\partial \widetilde{H}_i}{\partial c_j}\nonumber \\ \Longrightarrow \ \dot{\lambda }_{ij}(t)= & {} (\rho -\delta ) \lambda _{ij}(t), \ i,j=1, \ldots , h, \ i \ne j, \end{aligned}$$
(30)
$$\begin{aligned} \dot{\lambda }_{ij}(t)= & {} \rho \lambda _{ij}(t)-\dfrac{\partial \widetilde{H}_i}{\partial c_j}\nonumber \\ \Longrightarrow \ \dot{\lambda }_{ij}(t)= & {} (\rho -\delta ) \lambda _{ij}(t), \ i=1, \ldots , h, \ j=h+1, \ldots , N, \end{aligned}$$
(31)
$$\begin{aligned} \dot{\mu }_{ii}(t)= & {} \rho \mu _{ii}(t)-\dfrac{\partial \overline{H}_i}{\partial c_i}\nonumber \\ \Longrightarrow \ \dot{\mu }_{ii}(t)= & {} (\rho -\delta ) \mu _{ii}(t)+\dfrac{h \widetilde{c}(t)-(h+1)\overline{c}(t)+A}{N+1}, \ i=h+1, \ldots , N, \end{aligned}$$
(32)
$$\begin{aligned} \dot{\mu }_{ij}(t)= & {} \rho \mu _{ij}(t)-\dfrac{\partial \overline{H}_i}{\partial c_j}\nonumber \\ \Longrightarrow \ \dot{\mu }_{ij}(t)= & {} (\rho -\delta ) \mu _{ij}(t), \ i,j=h+1, \ldots , N, \ i \ne j, \end{aligned}$$
(33)
$$\begin{aligned} \dot{\mu }_{ij}(t)= & {} \rho \mu _{ij}(t)-\dfrac{\partial \overline{H}_i}{\partial c_j}\nonumber \\ \Longrightarrow \ \dot{\mu }_{ij}(t)= & {} (\rho -\delta ) \mu _{ij}(t), \ i=h+1, \ldots , N, \ j=1, \ldots , h. \end{aligned}$$
(34)

The associated transversality conditions are:

$$\begin{aligned}&\lim \limits _{t \rightarrow T_2} e^{-\rho t}\lambda _{ii}(t)c_i(t)=0, \end{aligned}$$
(35)
$$\begin{aligned}&\lim \limits _{t \rightarrow T_2} e^{-\rho t}\lambda _{ij}(t)c_j(t)=0, \end{aligned}$$
(36)

for \(i=1, \ldots , h\).

$$\begin{aligned}&\lim \limits _{t \rightarrow T_1} e^{-\rho t}\mu _{ii}(t)c_i(t)=0, \end{aligned}$$
(37)
$$\begin{aligned}&\lim \limits _{t \rightarrow T_1} e^{-\rho t}\mu _{ij}(t)c_j(t)=0, \end{aligned}$$
(38)

for \(i=h+1, \ldots , N\).

Note that the concavity of all Hamiltonian functions, with respect to the control variables, ensures that all the second-order conditions hold.

The costate equations deserve further investigation: Eqs. (30) and (33) are not actually relevant for the model dynamics, because the related costate variables do not appear in (11) and (13). On the other hand, (31) and (34) trivially admit the nil solutions \(\lambda _{ij}=\mu _{ij} \equiv 0\), but if such solutions were plugged into (11) and (13), then the spillover effects measured by \(\gamma \) would vanish in the strategic equations.

After inserting the optimal controls obtained in (11) and (13) into (29) and (32), we achieve the dynamic equations for the open-loop strategies of controls \(\widetilde{k}(t)\) and \(\overline{k}(t)\), thus entailing the state-control dynamic system (17), having initial conditions on marginal costs, i.e., \(\widetilde{c}(0)=\widetilde{c}_0\), \(\overline{c}(0)=\overline{c}_0\), and final conditions on Research & Development levels. This choice of final conditions is due to the transversality conditions: (36) and (38) trivially hold, because the related costate variables vanish at all t. On the other hand, (35) and (37) provide us with \(\widetilde{k}(T_1)=\overline{k}(T_1)=0\), because \(\lambda _{ii}\) and \(\mu _{ii}\) cannot be identically zero; otherwise, the model would collapse to a static game.

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Bramati, M.C., Palestini, A. & Rota, M. Effects of Law-Enforcement Efficiency and Duration of Trials in an Oligopolistic Competition Among Fair and Unfair Firms. J Optim Theory Appl 170, 650–669 (2016). https://doi.org/10.1007/s10957-016-0866-5

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