Skip to main content
Log in

The Role of Noise and Initial Conditions in the Asymptotic Solution of a Bounded Confidence, Continuous-Opinion Model

  • Published:
Journal of Statistical Physics Aims and scope Submit manuscript

Abstract

We study a model for continuous-opinion dynamics under bounded confidence. In particular, we analyze the importance of the initial distribution of opinions in determining the asymptotic configuration. Thus, we sketch the structure of attractors of the dynamical system, by means of the numerical computation of the time evolution of the agents density. We show that, for a given bound of confidence, a consensus can be encouraged or prevented by certain initial conditions. Furthermore, a noisy perturbation is added to the system with the purpose of modeling the free will of the agents. As a consequence, the importance of the initial condition is partially replaced by that of the statistical distribution of the noise. Nevertheless, we still find evidence of the influence of the initial state upon the final configuration for a short range of the bound of confidence parameter.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Fig. 1
Fig. 2
Fig. 3
Fig. 4
Fig. 5
Fig. 6
Fig. 7
Fig. 8
Fig. 9

Similar content being viewed by others

References

  1. Castellano, C., Fortunato, S., Loreto, V.: Rev. Mod. Phys. 81, 591 (2009)

    Article  ADS  Google Scholar 

  2. Lorenz, J.: Int. J. Mod. Phys. C 18, 1819 (2007)

    Article  ADS  MATH  Google Scholar 

  3. Hegselmann, R., Krause, U.: J. Artif. Soc. Soc. Simul. 5, 1 (2002)

    Google Scholar 

  4. Deffuant, G., Neau, D., Amblard, F., Weisbuch, G.: Adv. Complex Syst. 3, 87 (2000)

    Article  Google Scholar 

  5. Weisbuch, G., Deffuant, G., Amblard, F., Nadal, J.P.: Complexity 7(3), 55 (2002)

    Article  Google Scholar 

  6. Krause, U.: In: Elyadi, S., Ladas, G., Popenda, J., Rakowski, J. (eds.) Communications in Difference Equations, pp. 227–236. Gordon & Breach, Amsterdam (2000)

    Google Scholar 

  7. Pineda, M., Toral, R., Hernández-García, E.: J. Stat. Mech. Theory Exp. 2009(08), P08001 (2009)

    Article  Google Scholar 

  8. Pineda, M., Toral, R., Hernández-García, E.: Eur. Phys. J. D 62, 109 (2011)

    Article  ADS  Google Scholar 

  9. Ben-Naim, E., Krapivsky, P., Redner, S.: Physica D, Nonlinear Phenom. 183(3–4), 190 (2003)

    Article  MathSciNet  ADS  MATH  Google Scholar 

  10. Lorenz, J., Tonella, G.: In: Proceedings of the Fifth IASTED International Conference on Modelling, Simulation, and Optimization, pp. 61–66 (2005)

    Google Scholar 

  11. Laguna, M.F., Abramson, G., Zanette, D.H.: Complexity 9(4), 31 (2004)

    Article  MathSciNet  Google Scholar 

  12. Porfiri, M., Bollt, E.M., Stilwell, D.J.: Eur. Phys. J. B, Condens. Matter Complex Syst. 57, 481 (2007)

    Article  Google Scholar 

  13. Lorenz, J.: PHD Thesis, Universität Bremen (2007)

  14. Lorenz, J.: Complexity 15(4), 43 (2010)

    MathSciNet  Google Scholar 

  15. Mäs, M., Flache, A., Helbing, D.: PLoS Comput. Biol. 6(10), e1000959 (2010)

    Article  Google Scholar 

Download references

Acknowledgements

This work was supported by MINECO (Spain), Comunitat Autónoma de les Illes Balears, FEDER, and the European Commission under project FIS2007-60327. AC is supported by a PhD grant from the University of the Balearic Islands.

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Raúl Toral.

Appendix: Lyapunov Function for the DW et al. Model

Appendix: Lyapunov Function for the DW et al. Model

In order to write a Lyapunov function for the DW et al. process, we need to find a function , where x(t) is a vector whose components are the agents opinions at time t, which satisfies

(A.1)
(A.2)

where (A.1) simply means that it is a positive-definite function and (A.2) that it cannot increase with time.

We will first write a positive-definite function and then prove that it is decreasing in time for the model interaction rules. Let us write a function which only depends on the distances between the agents opinions as

(A.3)

where we only sum over all terms which are different. Let us then focus on one interaction, i.e., on the changes occurred to the positions of only two agents in the opinion space, say agents i 1 and j 1. Thus, we may divide the Lyapunov function into two terms, one dependent and the other independent of i 1 and j 1, and let us call A to the independent part for simplicity:

(A.4)

Each sum contains N−2 terms, being N the number of agents. Now we use the new opinions \(x_{i_{1}}(t+1)\) and \(x_{j_{1}}(t+1)\) that agents i 1 and j 1 hold after the interaction. It is important to notice that this interaction does only take place in case the opinions of the agents are nearer than the bound of confidence ε. However, this does not affect our analysis, as we are only interested in effective interactions, those which actually take place. The Lyapunov function after the interaction is

(A.5)

Replacing the new values \(x_{i_{1}}(t+1)\) and \(x_{j_{1}}(t+1)\) as given by application of the rule Eq. (1) and subtracting, we get the variation of the Lyapunov as which, after some algebra, reads:

(A.6)

Therefore, we see that the Lyapunov function is strictly decreasing in time when any interaction takes place, and it stays constant when no interaction occurs.

Rights and permissions

Reprints and permissions

About this article

Cite this article

Carro, A., Toral, R. & San Miguel, M. The Role of Noise and Initial Conditions in the Asymptotic Solution of a Bounded Confidence, Continuous-Opinion Model. J Stat Phys 151, 131–149 (2013). https://doi.org/10.1007/s10955-012-0635-2

Download citation

  • Received:

  • Accepted:

  • Published:

  • Issue Date:

  • DOI: https://doi.org/10.1007/s10955-012-0635-2

Keywords

Navigation