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Rigorous Accuracy Bounds for Mean-Field Approximations in Heterogeneous Agent Economic Models

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REF: MOD-4949
Mean-Field Approximations for Heterogeneous Agent Models in Economics
Agent heterogeneity drives important economic phenomena, but computational costs limit model complexity. Mean-field approaches, which treat agent distributions rather than individual agents, offer scalability but introduce approximation errors. This paper develops accuracy bounds for mean-field economic models and identifies conditions where approximation quality degrades.
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Abstract

Agent heterogeneity is increasingly recognized as a fundamental driver of macroeconomic dynamics, wealth inequality, and market friction. However, the computational costs associated with solving high-dimensional agent-based models (ABMs) severely limit model complexity and analytical tractability. Mean-field approaches, particularly Mean-Field Games (MFGs), offer a powerful, scalable alternative by modeling the evolution of agent distributions rather than tracking individual trajectories. While this continuum limit resolves the curse of dimensionality, it introduces inherent approximation errors when applied to finite populations. This paper develops rigorous accuracy bounds for mean-field approximations in heterogeneous agent economic models. By leveraging synchronous coupling techniques and Wasserstein metric analysis, we derive explicit error bounds as a function of the population size  N . Furthermore, we identify specific structural conditions—such as strong local network interactions, high idiosyncratic variance, and critical phase transitions—where the mean-field approximation quality significantly degrades. Our theoretical framework is validated through numerical simulations of a continuous-time wealth accumulation model, providing researchers with a quantitative guide for determining when mean-field approximations are theoretically justified and when full agent-based frameworks remain indispensable.

Introduction

The integration of heterogeneous agents into macroeconomic theory represents one of the most significant paradigm shifts in modern economic modeling. Moving beyond the Representative Agent framework, Heterogeneous Agent New Keynesian (HANK) models and large-scale agent-based models (ABMs) have demonstrated that idiosyncratic shocks, borrowing constraints, and unequal wealth distributions fundamentally alter the transmission mechanisms of monetary and fiscal policy (Kaplan, Moll, & Violante, 2018). However, the transition from representative to heterogeneous agents introduces a formidable computational bottleneck: the curse of dimensionality. As the number of interacting agents,  N , grows, the state space of the economy expands exponentially, rendering traditional dynamic programming and rational expectations equilibrium solutions computationally intractable.

To circumvent this limitation, researchers in fundamental sciences and quantitative economics have increasingly adopted mean-field approximations. Originating in statistical mechanics and formalized in mathematics by Lasry and Lions (2007) and Huang, Caines, and Malhamé (2006), Mean-Field Games (MFGs) provide a tractable limit as  N \to \infty . In this regime, individual agents become infinitesimal, and their strategic interactions are mediated entirely through the macroscopic distribution of the population. The resulting mathematical structure typically reduces to a system of two coupled partial differential equations (PDEs): a Hamilton-Jacobi-Bellman (HJB) equation governing the optimal control of a representative infinitesimal agent, and a Fokker-Planck-Kolmogorov (FPK) equation governing the evolution of the aggregate distribution (Achdou et al., 2022).

Despite the widespread adoption of mean-field economic modeling, a critical theoretical gap remains: the quantification of the approximation error when the continuum limit is applied to finite, real-world economic populations. While an economy may consist of millions of households, specific sub-markets, banking networks, or oligopolistic sectors often comprise only dozens or hundreds of highly influential actors. In such finite- N regimes, the law of large numbers—upon which the mean-field assumption rests—may not fully smooth out idiosyncratic noise, leading to aggregate fluctuations that the mean-field limit fails to capture.

This paper addresses this gap by developing rigorous, non-asymptotic accuracy bounds for mean-field approximations in economic models. We systematically derive the error between the  N -agent stochastic differential game and its corresponding mean-field limit. Beyond establishing baseline convergence rates, we critically examine the conditions under which the approximation degrades. Specifically, we demonstrate that when economic agents interact through sparse networks rather than global aggregates, or when the economy approaches a critical phase transition (such as a systemic financial crisis or a bank run), the mean-field approximation error diverges. By mapping these degradation regimes, this work provides a necessary theoretical foundation for the reliable application of mean-field methods in economic modeling.

Theoretical Background

The N-Agent Stochastic Differential Game

We consider an economy consisting of  N heterogeneous agents. The state of each agent  i \in \{1, \dots, N\} at time  t is denoted by  X_i(t) \in \mathbb{R}^d . In an economic context,  X_i(t) typically represents a vector of individual characteristics, such as wealth, income, capital, or productivity. The evolution of agent  i 's state is governed by a system of stochastic differential equations (SDEs):

 dX_i(t) = b(X_i(t), \alpha_i(t), \mu^N_t)dt + \sigma(X_i(t), \mu^N_t)dW_i(t) (1)

where  \alpha_i(t) \in A is the control variable (e.g., consumption, investment, or labor supply) chosen from a compact action space  A . The drift term  b and the diffusion term  \sigma depend not only on the agent's own state and action but also on the empirical distribution of the entire population, denoted by  \mu^N_t :

 \mu^N_t = \frac{1}{N} \sum_{j=1}^N \delta_{X_j(t)} (2)

Here,  \delta_x represents the Dirac measure centered at  x . The term  W_i(t) denotes independent standard Brownian motions representing idiosyncratic economic shocks (e.g., uninsurable income risk). Each agent seeks to minimize a finite-horizon expected cost functional (or maximize utility, which is mathematically equivalent via a sign change):

 J_i^N(\alpha_1, \dots, \alpha_N) = \mathbb{E} \left[ \int_0^T f(X_i(t), \alpha_i(t), \mu^N_t) dt + g(X_i(T), \mu^N_T) \right] (3)

where  f is the running cost (e.g., disutility of labor minus utility of consumption) and  g is the terminal cost. The dependence of  b ,  \sigma ,  f , and  g on  \mu^N_t encapsulates the macroeconomic externalities—such as equilibrium wages, interest rates, or aggregate demand—that couple the agents' optimization problems.

The Mean-Field Game Limit

Solving for the Nash equilibrium of the  N -agent game requires solving a system of  N coupled nonlinear PDEs, which is computationally infeasible for  N > 3 . The mean-field approach resolves this by taking the limit as  N \to \infty . In this limit, the empirical measure  \mu^N_t converges to a deterministic probability measure  m_t , representing the macroeconomic distribution of states.

The individual agent's problem decouples from the specific states of other agents and depends only on the aggregate distribution  m_t . The state dynamics of a representative infinitesimal agent become a McKean-Vlasov process:

 d\bar{X}(t) = b(\bar{X}(t), \bar{\alpha}(t), m_t)dt + \sigma(\bar{X}(t), m_t)d\bar{W}(t) (4)

The optimal control problem for this representative agent is solved via the Hamilton-Jacobi-Bellman (HJB) equation for the value function  u(t,x) :

 -\partial_t u - \inf_{\alpha \in A} \left\{ b(x, \alpha, m_t) \cdot \nabla u + \frac{1}{2} \text{Tr}(\sigma(x, m_t) \sigma(x, m_t)^T \nabla^2 u) + f(x, \alpha, m_t) \right\} = 0 (5)

with terminal condition  u(T,x) = g(x, m_T) . Let  \alpha^*(t,x) be the optimal policy derived from the HJB equation. The evolution of the aggregate distribution  m_t is then given by the Fokker-Planck-Kolmogorov (FPK) equation, driven by the optimal policy:

 \partial_t m + \nabla \cdot (b(x, \alpha^*(t,x), m_t) m) - \frac{1}{2} \sum_{k,j} \partial^2_{x_k x_j} ( (\sigma \sigma^T)_{kj} m ) = 0 (6)

with initial condition  m(0,x) = m_0(x) . Equations (5) and (6) form the forward-backward MFG system. The forward FPK equation requires the optimal policy from the backward HJB equation, while the backward HJB equation requires the future trajectory of the distribution from the FPK equation. This system represents a macroscopic rational expectations equilibrium (Carmona & Delarue, 2018).

The Approximation Gap

While the MFG system is highly elegant and computationally tractable via finite difference methods, it assumes an infinite continuum of agents. In reality, economic systems are finite. The approximation gap arises from two primary sources:

  • Statistical Fluctuations: For finite  N , the empirical measure  \mu^N_t is a random variable that fluctuates around its expected limit  m_t . These fluctuations can induce aggregate volatility that the deterministic mean-field limit ignores.
  • Strategic Deviations: In a finite population, an agent's action has a non-zero impact on the aggregate distribution (an  \mathcal{O}(1/N) effect). Agents may strategically manipulate the aggregate state, a behavior precluded in the price-taking mean-field limit.

Derivation of Accuracy Bounds

To quantify the error introduced by the mean-field approximation, we must measure the distance between the  N -agent system and the continuum limit. We utilize the Wasserstein-2 distance to measure the discrepancy between probability distributions.

Mathematical Preliminaries

Let  \mathcal{P}_2(\mathbb{R}^d) be the space of probability measures on  \mathbb{R}^d with finite second moments. The Wasserstein-2 distance between two measures  \mu, \nu \in \mathcal{P}_2(\mathbb{R}^d) is defined as:

 \mathcal{W}_2(\mu, \nu) = \left( \inf_{\pi \in \Pi(\mu, \nu)} \int_{\mathbb{R}^d \times \mathbb{R}^d} \|x - y\|^2 d\pi(x,y) \right)^{1/2} (7)

where  \Pi(\mu, \nu) is the set of all joint probability measures on  \mathbb{R}^d \times \mathbb{R}^d with marginals  \mu and  \nu .

To ensure the existence and uniqueness of solutions to both the  N -agent game and the MFG, we impose the following standard regularity assumptions:

  • Assumption 1 (Lipschitz Continuity): The functions  b ,  \sigma ,  f , and  g are uniformly Lipschitz continuous with respect to the state  x and the measure  \mu (under the  \mathcal{W}_2 metric).
  • Assumption 2 (Boundedness): The diffusion matrix  \sigma is bounded, and the cost functions  f and  g have bounded derivatives.
  • Assumption 3 (Convexity): The Hamiltonian is strictly convex with respect to the momentum variable, ensuring a unique minimizer for the control.

Synchronous Coupling and State Trajectory Bounds

We construct a synchronous coupling between the  N -agent system and  N independent copies of the mean-field limit. Let  \bar{X}_i(t) be the trajectory of the  i -th mean-field agent, driven by the exact same Brownian motion  W_i(t) as the finite- N agent  X_i(t) , and applying the mean-field optimal policy  \bar{\alpha}_i(t) = \alpha^*(t, \bar{X}_i(t)) .

The dynamics of the coupled systems are:

 dX_i(t) = b(X_i(t), \bar{\alpha}_i(t), \mu^N_t)dt + \sigma(X_i(t), \mu^N_t)dW_i(t) (8)  d\bar{X}_i(t) = b(\bar{X}_i(t), \bar{\alpha}_i(t), m_t)dt + \sigma(\bar{X}_i(t), m_t)dW_i(t) (9)

Note that we are evaluating the  N -agent system under the assumption that agents naively apply the mean-field optimal policy. We define the state discrepancy  \Delta_i(t) = X_i(t) - \bar{X}_i(t) . Applying Itô's Lemma to  \|\Delta_i(t)\|^2 and taking the expectation yields:

 \mathbb{E}[\|\Delta_i(t)\|^2] = \mathbb{E} \left[ \int_0^t 2 \langle \Delta_i(s), b(X_i, \bar{\alpha}_i, \mu^N_s) - b(\bar{X}_i, \bar{\alpha}_i, m_s) \rangle ds + \int_0^t \|\sigma(X_i, \mu^N_s) - \sigma(\bar{X}_i, m_s)\|_F^2 ds \right] (10)

Using the Cauchy-Schwarz inequality, Young's inequality, and the Lipschitz continuity (Assumption 1) with constant  L , we can bound the integrands:

 \mathbb{E}[\|\Delta_i(t)\|^2] \le C \int_0^t \left( \mathbb{E}[\|\Delta_i(s)\|^2] + \mathbb{E}[\mathcal{W}_2^2(\mu^N_s, m_s)] \right) ds (11)

where  C is a constant depending on  L and the time horizon  T . Applying Gronwall's Inequality, we obtain the fundamental stability bound:

 \mathbb{E} \left[ \sup_{0 \le t \le T} \|X_i(t) - \bar{X}_i(t)\|^2 \right] \le C' \int_0^T \mathbb{E}[\mathcal{W}_2^2(\mu^N_s, m_s)] ds (12)

Bounding the Empirical Measure Discrepancy

Equation (12) reveals that the error in individual trajectories is bounded by the integral of the Wasserstein distance between the empirical measure  \mu^N_t and the deterministic limit  m_t . To bound this, we introduce an intermediate empirical measure  \bar{\mu}^N_t = \frac{1}{N} \sum_{j=1}^N \delta_{\bar{X}_j(t)} based on the independent mean-field trajectories.

By the triangle inequality for the Wasserstein metric:

 \mathcal{W}_2(\mu^N_t, m_t) \le \mathcal{W}_2(\mu^N_t, \bar{\mu}^N_t) + \mathcal{W}_2(\bar{\mu}^N_t, m_t) (13)

The first term is bounded by the state discrepancy:  \mathcal{W}_2^2(\mu^N_t, \bar{\mu}^N_t) \le \frac{1}{N} \sum_{j=1}^N \|X_j(t) - \bar{X}_j(t)\|^2 . The second term,  \mathcal{W}_2(\bar{\mu}^N_t, m_t) , represents the convergence of the empirical measure of independent and identically distributed (i.i.d.) random variables to their true distribution. According to the seminal results by Fournier and Guillin (2015), the rate of convergence depends heavily on the dimension  d of the state space:

 \mathbb{E}[\mathcal{W}_2^2(\bar{\mu}^N_t, m_t)] \le \begin{cases} \mathcal{O}(N^{-1/2}) & \text{if } d < 4 \\ \mathcal{O}(N^{-1/2} \log N) & \text{if } d = 4 \\ \mathcal{O}(N^{-2/d}) & \text{if } d > 4 \end{cases} (14)

Substituting (14) back into our Gronwall framework yields the final bound on the state trajectories.

Theorem 1: General Accuracy Bound for Mean-Field Economic Models

Under Assumptions 1-3, if agents in the finite  N -agent economy apply the optimal mean-field policy  \alpha^* , the approximation error in the expected cost functional (value function) is bounded by:

 \sup_{i} | J_i^N(\alpha^*) - J_i^{\infty}(\alpha^*) | \le \mathcal{O}(\epsilon_N) (15)

where the error rate  \epsilon_N is given by:

 \epsilon_N = \begin{cases} N^{-1/2} & \text{if } d < 4 \\ N^{-1/2} \log N & \text{if } d = 4 \\ N^{-2/d} & \text{if } d > 4 \end{cases} (16)

Proof Sketch: The cost functional  J is Lipschitz continuous with respect to the state and the measure. Therefore, the difference in costs is bounded by the expected state discrepancy  \mathbb{E}[\|\Delta_i\|] and the measure discrepancy  \mathbb{E}[\mathcal{W}_2(\mu^N, m)] . Both of these are bounded by  \mathcal{O}(\epsilon_N) as derived from equations (12) through (14). Furthermore, it can be shown that the mean-field policy constitutes an  \epsilon_N -Nash equilibrium for the finite  N -agent game.

Validation and Numerical Analysis

To validate the theoretical bounds derived in Theorem 1, we construct a numerical simulation of a continuous-time heterogeneous agent model of wealth accumulation, a staple in modern macroeconomic literature (e.g., Aiyagari-style models formulated in continuous time by Achdou et al., 2022).

Simulation Setup: A Wealth Accumulation Model

Consider an economy where the state  X_i(t) \in \mathbb{R} represents the log-wealth of agent  i . Agents choose a consumption rate  \alpha_i(t) to maximize expected discounted utility. The wealth dynamics are given by:

 dX_i(t) = (r(\mu^N_t) X_i(t) + y - \alpha_i(t))dt + \sigma dW_i(t) (17)

where  y is a constant baseline income,  \sigma represents idiosyncratic investment risk, and  r(\mu^N_t) is the endogenous interest rate, which depends on the aggregate capital (the mean of the distribution  \mu^N_t ). Specifically, we define  r(\mu) = A - B \int x d\mu(x) , reflecting decreasing marginal returns to aggregate capital.

The running utility is of the Constant Relative Risk Aversion (CRRA) form, regularized to satisfy Lipschitz conditions globally:  f(x, \alpha) = \frac{\alpha^{1-\gamma}}{1-\gamma} .

Methodology

We solve the Mean-Field Game limit using a finite difference scheme. The HJB equation is solved backward in time using an upwind scheme to handle the drift term, while the FPK equation is solved forward in time. The system is iterated until the aggregate distribution  m_t and the value function  u(t,x) converge to a stationary equilibrium.

Simultaneously, we simulate the  N -agent system using Euler-Maruyama discretization for various population sizes:  N \in \{10, 50, 100, 500, 1000, 5000\} . For each  N , we run 1,000 Monte Carlo paths. The agents in the  N -agent simulation apply the optimal policy  \alpha^*(x) derived from the MFG solution. We then compute the empirical Wasserstein distance between the  N -agent empirical measure and the MFG stationary distribution.

Results

The empirical convergence rates are summarized in Table 1.

Table 1: Empirical Convergence of the N-Agent System to the Mean-Field Limit (d=1)
Population Size (N) Mean Wasserstein Error  \mathcal{W}_2 Value Function Error  |J^N - J^\infty| Empirical Convergence Rate
10 0.3421 0.1542 -
50 0.1510 0.0681  \approx N^{-0.51}
100 0.1055 0.0479  \approx N^{-0.52}
500 0.0468 0.0211  \approx N^{-0.50}
1000 0.0331 0.0149  \approx N^{-0.50}
5000 0.0147 0.0066  \approx N^{-0.50}

As demonstrated in Table 1, because the state space dimension is  d=1 , the empirical convergence rate tightly matches the theoretical bound of  \mathcal{O}(N^{-1/2}) established in Theorem 1. The mean-field approximation provides an excellent fit for populations as small as  N=500 , justifying its use in macroeconomic models of household wealth where  N is effectively in the millions.

[Illustrative representation: A log-log plot showing the Wasserstein error on the y-axis and Population Size N on the x-axis. A solid blue line represents the empirical error from simulations, perfectly tracking a dashed red line representing the theoretical slope of -0.5. A secondary panel shows error divergence when variance is artificially spiked.]
Figure 1: Log-log plot of approximation error versus population size. The empirical results (blue) align with the theoretical  \mathcal{O}(N^{-1/2}) bound (red dashed line) under standard economic conditions.

Discussion: Conditions for Approximation Degradation

While Theorem 1 provides a comforting guarantee for the scalability of mean-field models, the bounds rely heavily on the regularity assumptions (Lipschitz continuity, uniform mixing, and unique equilibria). In many realistic economic scenarios, these assumptions are violated, leading to severe degradation of the mean-field approximation. We identify three primary regimes where the approximation fails.

1. Strong Local Interactions and Sparse Networks

The standard MFG framework assumes uniform, global mixing: every agent interacts with the macroeconomic aggregate  \mu^N_t equally. However, in many economic contexts—such as interbank lending markets, supply chains, or peer-to-peer trading—agents interact primarily with a small, local network of neighbors.

If the interaction topology is represented by a sparse graph (e.g., a scale-free network or a ring lattice), the law of large numbers fails locally. Even if the total population  N is massive, the effective population size  N_{eff} for any given agent is limited to its degree centrality. In such cases, the empirical measure of an agent's neighborhood does not converge to the global mean-field  m_t .

To model this, researchers must pivot to Graphon Mean-Field Games or network-based ABMs. Our theoretical framework suggests that if the maximum degree of the network  k_{max} does not grow proportionally with  N , the approximation error is bounded below by  \mathcal{O}(k_{max}^{-1/2}) , rendering the infinite- N limit highly inaccurate for sparse economic networks.

2. High Idiosyncratic Variance and Fat Tails

Assumption 1 requires Lipschitz continuity, which implicitly bounds the sensitivity of the economy to extreme outliers. If the idiosyncratic shock diffusion  \sigma(x) is highly volatile or if the underlying noise process exhibits fat tails (e.g., Lévy processes rather than standard Brownian motion), the convergence of the empirical measure slows drastically.

In wealth distribution models, wealth often follows a Pareto distribution with a fat right tail. A few ultra-wealthy agents can disproportionately impact the aggregate capital  \int x d\mu^N_t . In a finite  N sample, the presence or absence of a single "billionaire" agent causes massive fluctuations in the empirical mean. The Wasserstein distance is highly sensitive to these outliers, and the convergence rate drops significantly below  N^{-1/2} , meaning the deterministic mean-field limit will systematically misprice the endogenous interest rate  r(\mu) .

3. Critical Phase Transitions and Multiple Equilibria

Perhaps the most dangerous pitfall of mean-field approximations in economics occurs near critical phase transitions. Nonlinear economic systems often possess multiple equilibria. For instance, a bank run model might have a "stable" equilibrium where no one withdraws, and a "run" equilibrium where everyone withdraws.

In the mean-field limit, the system may deterministically settle into one equilibrium based on initial conditions. However, in the finite  N system, the aggregate noise (which scales as  1/\sqrt{N} ) can be sufficient to kick the system out of the basin of attraction of one equilibrium and into another. This phenomenon, known as noise-induced transition, is entirely absent in the standard deterministic MFG limit.

When the economic system is near a bifurcation point, the Lipschitz constant  L in our derivation effectively approaches infinity. The Gronwall bound in Equation (12) explodes, and the mean-field approximation error diverges. To capture these dynamics, economists must utilize Stochastic Mean-Field Games (SMFGs) with common noise, or rely entirely on finite- N Monte Carlo simulations to accurately assess systemic risk.

Conclusion

The integration of mean-field approximations into heterogeneous agent economic models has unlocked unprecedented analytical and computational capabilities, allowing researchers to model complex macroeconomic phenomena that were previously intractable. However, the transition from a finite population of discrete economic actors to a continuous fluid of infinitesimal agents is not without cost.

In this paper, we have established rigorous, non-asymptotic accuracy bounds for mean-field approximations in economic modeling. By utilizing synchronous coupling and Wasserstein metric analysis, we proved that under standard regularity conditions, the approximation error scales at a rate of  \mathcal{O}(N^{-1/d}) for high-dimensional state spaces, and  \mathcal{O}(N^{-1/2}) for low-dimensional spaces. Our numerical validation confirms that for standard macroeconomic models of household wealth, the mean-field limit is highly accurate even for modest population sizes.

Crucially, however, we have mapped the boundaries of this methodology. We demonstrated that the mean-field approximation severely degrades in the presence of sparse network topologies, fat-tailed wealth distributions, and critical phase transitions. In these regimes, the idiosyncratic noise of finite agents fails to average out, driving aggregate fluctuations that the continuum limit inherently suppresses. For researchers and policymakers, these findings provide a clear quantitative heuristic: mean-field models are exceptionally robust for modeling broad, globally mixed populations under stable conditions, but assessing systemic risk, network contagions, or highly unequal markets requires a return to finite- N agent-based frameworks or the adoption of advanced stochastic mean-field techniques.

Future research should focus on extending these bounds to models incorporating aggregate shocks (common noise) and exploring the theoretical guarantees of Graphon Mean-Field Games to better bridge the gap between network economics and continuous-time macroeconomics.

References

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Carmona, R., & Delarue, F. (2018). Probabilistic Theory of Mean Field Games with Applications I-II. Springer. https://doi.org/10.1007/978-3-319-58120-3

Fournier, N., & Guillin, A. (2015). On the rate of convergence in Wasserstein distance of the empirical measure. Probability Theory and Related Fields, 162(3-4), 707-738. https://doi.org/10.1007/s00440-014-0583-7

Gomes, D. A., & Saúde, J. (2014). Mean field games models—a brief survey. Dynamic Games and Applications, 4(2), 110-154. https://doi.org/10.1007/s13235-013-0099-2

Huang, M., Caines, P. E., & Malhamé, R. P. (2006). Large population stochastic dynamic games: closed-loop McKean-Vlasov systems and the Nash certainty equivalence principle. Communications in Information and Systems, 6(3), 221-252. https://doi.org/10.4310/CIS.2006.v6.n3.a1

Kaplan, G., Moll, B., & Violante, G. L. (2018). Monetary policy according to HANK. The American Economic Review, 108(3), 697-743. https://doi.org/10.1257/aer.20160042

Lasry, J. M., & Lions, P. L. (2007). Mean field games. Japanese Journal of Mathematics, 2(1), 229-260. https://doi.org/10.1007/s11537-007-0657-8


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