A closer look at coupled logistic maps at the edge of chaos

A closer look at coupled logistic maps at the edge of chaos

Ugur Tirnakli ugur.tirnakli@ege.edu.tr Department of Physics, Faculty of Science, Ege University, 35100 Izmir, Turkey    Constantino Tsallis tsallis@cbpf.br Centro Brasileiro de Pesquisas Físicas and National Institute for Science and Technology of Complex Systems, Rua Dr. Xavier Sigaud 150, 22290-180 Rio de Janeiro, RJ, Brazil
and
Santa Fe Institute, 1399 Hyde Park Road, Santa Fe, NM 87501, USA
July 3, 2019
Abstract

We focus on a linear chain of first-neighbor-coupled logistic maps at their edge of chaos in the presence of a common noise. This model, characterised by the coupling strength and the noise width , was recently introduced by Pluchino et al [Phys. Rev. E 87, 022910 (2013)]. They detected, for the time averaged returns with characteristic return time , possible connections with -Gaussians, the distributions which optimise, under appropriate constraints, the nonadditive entropy , basis of nonextensive statistics mechanics. We have here a closer look on this model, and numerically obtain probability distributions which exhibit a slight asymmetry for some parameter values, in variance with simple -Gaussians. Nevertheless, along many decades, the fitting with -Gaussians turns out to be numerically very satisfactory for wide regions of the parameter values, and we illustrate how the index evolves with . It is nevertheless instructive on how careful one must be in such numerical analysis. The overall work shows that physical and/or biological systems that are correctly mimicked by the Pluchino et al model are thermostatistically related to nonextensive statistical mechanics when time-averaged relevant quantities are studied.

pacs:
05.45.Ra, 74.40.De, 87.19.lm

I Introduction

Synchronization has long been observed in complex systems and extensively studied in the literature synch1 (); synch2 (). In these studies, coupled maps are considered as an important theoretical model for these systems kaneko (). Moreover, since many biological systems evolve in noisy environments, it is important to analyse the effect of noise in such coupled maps. Recently, the effect of weak noise on globally coupled chaotic units has been studied for several systems kaneko2 (); kuramoto ().

The model that we focus on here is a linear chain of coupled logistic maps, with periodic boundary conditions, and can be written as

(1)

where is the local coupling, and is an additive random noise uniformly distributed in , which fluctuates in time but is equal for all maps. Here, the th logistic map at any time is given as

(2)

where is the map parameter and this function is taken in module 1 with sign in order to fold the iterates of the maps back into the map interval if the noise takes them out of this interval. All elements of the system will be kept at the chaos threshold by fixing the parameter at .

Very recently, the probability distribution functions (PDFs) of the returns for this model have been investigated numerically by Pluchino et al.Alex2013 () and fat-tailed distributions have been reported, which can be fitted by -Gaussians. The physical quantity under investigation, the returns, is a commonly used one in areas such as turbulence turbulence (), finance finance (); finance2 (), DNA sequences DNA (), and earthquake dynamics caruso (); bakar1 (); bakar2 (); ahmet () in the literature. It is defined as

(3)

where

(4)
Figure 1: Probability distribution functions of the normalized returns for logistic maps at the edge of chaos with . The parameter values used here are exactly those of Fig. 3a (case (a)) and of Fig. 3d (case (b)) of Alex2013 (). By expr we mean that only one experiment has been done in each of these illustrations.

The main result of Alex2013 () has been given in Fig. 3 of that paper where the PDFs of the normalized returns (normalized to the standard deviation of the overall sequence) have been plotted for various values. We have reproduced here in our Fig. 1 two representative cases, namely, and to be compared with Fig. 3a and Fig. 3d of Alex2013 (), respectively. It is evident that the -Gaussian curves with predicted values are very reasonable for these examples ( for and for ). However, the distributions span less than 3 decades since the time series that have been used are relatively short (). Therefore it is interesting to check the behaviour with longer time series in order to span more decades of the PDF. This is what we have done: see Fig. 2, which has been obtained by considering a large number of experiments (250 and 500). This means that the time series analysed are as long as and respectively. As seen clearly from Fig. 2, when one more decade is exhibited for the tails, the departure from the a priori admissible -Gaussians becomes clearly visible.

Figure 2: Probability distribution functions of the normalized returns for logistic maps at the edge of chaos with for (a) and (b). In order to analyse the tails of the distribution, large number of experiments is used. The size of the time series therefore equals to the number of experiments times the time steps used in each experiment (i.e., expr).

In addition to this, it is also interesting to check whether these typical numerical PDFs are asymptotic in the sense of the limit. If this is the case, one would expect the PDF curves to remain basically invariant as the size of the system increases. We have checked it: see two illustrative cases in Fig. 3. It is easily seen that the size cannot be considered as sufficient for the analysis of the asymptotic behaviour, especially for small values of .

Figure 3: Probability distribution functions of the normalized returns for logistic maps at the edge of chaos with for , and . It is evident that, as increases, the asymptotic PDFs are attained slowly for small values (i.e., case (a)), whereas it is quite quick for larger values (i.e., case (b)).

It is therefore clear at this stage that, if we are particularly interested in studying the asymptotic behaviour of PDFs of the normalized returns of this system, both the size of the system and the length of the time series must be quite large. To further refine numerically the present analysis, we have also studied the same two cases with large enough value for ( for . and for ), and with a time series of steps. These conditions are sufficient to observe the behaviour up to almost 6 decades. The results are given in Fig. 4. The strong departure from the -Gaussians with early predicted values becomes now very obvious. Moreover, a slight but neat asymmetry emerges for small . In order to fit this kind of behavior, one can use a non-symmetric extension of -Gaussian, namely given by

(5)

or even

(6)

These expressions recover the symmetric -Gaussian for . Strictly speaking, the case and is mathematically inadmissible since it would lead to a runaway to infinity. In contrast, the case and is perfectly admissible. However, in practice, unless we explore very large values of , we can consider with no sensible damage. A very good fitting has been obtained by using , , (with ) as illustrated in Fig. 4a. The representation of the same data using the -logarithmic function, defined as , has also been given in Fig. 4b. We notice that, in the asymptotic regime, the PDF for large values approaches a -Gaussian with , rather than a Gaussian, as first advanced in Ref.Alex2013 () far from the asymptotic regime: see Figs. 4c and 4d.

Figure 4: Asymptotic PDFs of the normalized returns with large and large number of time steps for (a) and (c). For both cases . The -logarithms versus the square of normalized returns have already been given for both cases in (b) and (d) respectively.

Ii -Gaussian approximants

Let us now attempt a wider look at the same problem, by extending the preliminary results given in Alex2013 (). A simple -Gaussian approximant describes fairly well the numerical data unless we focus on a parameter value where an asymmetry emerges in the PDF. The index is generically expected to depend on .

First of all, we need to define the procedure that we are employing in order to predict the best value of parameter of the related -Gaussian at each tuple. The -Gaussians can be obtained by optimising the entropy tsallis1 () and can be given for as

(7)

where , known as -exponential, is defined by

(8)

By inverting this function we obtain the -logarithm function defined above.

The -dependent coefficient in Eq. (7) is given by

(9)

The quantity characterizes the PDF width of the distribution as follows:

(10)

where is, for , related to the standard deviation through

(11)

In our simulations, there are only two free parameters, namely and , to be adjusted under the assumption that the number of decades that we are observing still shows a symmetric PDF. For a given set , we adjust the best value of by looking at the curves (PDF) versus (normalized returns). The procedure consists in determining the value of which provides the best approach to a straight line. More precisely, we fit the curves resulting from various values of with a quadratic function

(12)

and choose the value of which provides the minimal value for the parameter . Then, for this value, we calculate and parameters from the time series. Finally, using all these obtained parameter values, we plot the best -Gaussian for the chosen set . Two typical examples are given in Fig. 5. For these examples, the minimal value of , denoted by , have been obtained for and , respectively. Then these values of have been used to determine the values of the and parameters. Finally, the PDFs of the normalized returns are approached as shown in Fig. 5b and 5d. It is evident from the figure that the best -Gaussian approximants corroborate the behaviour of the system for more than 6 decades in each case. The obtained results are summarized in Table I and plotted in Fig. 6 for typical values of . Unless the values are very small, the tendency is always towards a -Gaussian with . For very small , are also observed but for such cases the asymmetry becomes important.

In our simulations, we prefer to set since it is evident from Fig. 7 that if is not very small the PDF remains the same as is increased.

Figure 5: Two typical examples of choosing the most appropriate value using the quadratic function for a case (a) and for a case (c). The appropriate value is taken as the one that gives the smallest value (denoted as ). The probability density of the same examples using the value obtained from the explained procedure for the case (b) and for the case (d).
0.001 0.4023 0.5171 1.022
0.05 0.3957 0.4840 0.978
0.1 0.3989 0.4897 0.986
0.2 0.3944 0.4771 0.968
0.3 0.3944 0.4771 0.968
0.4 0.3953 0.4819 0.975
0.5 0.3938 0.4744 0.964
0.6 0.3937 0.4737 0.963
0.7 0.3930 0.4704 0.958
0.0015 0.4214 0.6154 1.125
0.02 0.4077 0.5441 1.054
0.15 0.3912 0.4613 0.944
0.2 0.3888 0.4494 0.925
0.3 0.3926 0.4684 0.955
0.4 0.3912 0.4613 0.944
0.45 0.3885 0.4482 0.923
0.5 0.3873 0.4423 0.913
0.55 0.3950 0.4805 0.973
Table 1: For and two typical values of , the values of the parameters , and as varies are indicated.
Figure 6: The behaviour of the index as a function of for two typical values of .
Figure 7: The effect of on the behavior of the PDF.

We have also checked the effect of for a fixed value of . A clear tendency of increasing values as is decreasing has been observed with a saturation value around as given in Table II and plotted in Fig. 8.

0.000001 0.3938 0.4744 0.964
0.00001 0.3937 0.4737 0.963
0.0001 0.3941 0.4757 0.966
0.001 0.3939 0.4751 0.965
0.01 0.3939 0.4751 0.965
0.1 0.3914 0.4625 0.946
0.2 0.3895 0.4531 0.931
0.5 0.3878 0.4446 0.917
0.8 0.3873 0.4423 0.913
Table 2: For and a typical value of , the values of the parameters , and as varies are indicated.
Figure 8: The behaviour of the index as a function of for a typical value of .

Finally, we have simulated the case without noise. As expected, in this case, a clear Gaussian with 6 decades can be seen in Fig. 9 since all individual logistic maps are at their mostly chaotic points. Whenever a nonzero noise term is included, the system is not able to achieve the Gaussian due to the persistence of the noise on each map.

Figure 9: The behaviour of the PDF for a typical case of .

Iii Conclusions

We have numerically studied, along many decades, the time-averaged returns in the model recently introduced in Alex2013 () by varying the number of logistic maps in the chain, the first-neigbour-coupling constant , the width of the common noise, and the characteristic return time .

Our results can be summarised as follows. When the control parameter of the logistic maps is taken to be close to the edge of chaos (), where the Lyapunov exponent vanishes, slightly asymmetric distributions are observed for some parameter values. Unless the number of decades is quite large, this asymmetry can be neglected and the distributions satisfactorily admit -Gaussian approximants even for these parameter values. We have illustrated the effect on the index of the various parameters of the model.

When we choose for the parameter of the logistic maps not its value at the edge of chaos but any other value such that the Lyapunov exponent is positive, we obtain numerical PDFs that, as expected, are well fitted by simple Gaussians along six PDF decades when the system has no noise. In the presense of noise, however, the system is unable to achieve the Gaussian PDF due to the persistent perturbation of the noise.

The overall scenario is that, when we consider time-averaged relevant quantities such as the returns, Boltzmann-Gibbs statistics (with its Gaussians, consistent with the classical Central Limit Theorem) emerges when strong chaos (positive Lyapunov exponent) is present, and nonextensive statistical mechanics (with its -Gaussians, consistent with the -generalized Central Limit Theorem qCLT ()) emerges, or nearly emerges, when weak chaos (zero Lyapunov exponent) is present. These facts reinforce the results recently obtained with time-averaged quantities for the (conservative) standard map TirnakliBorges2014 (). Biological and other systems appear to be well mimicked by the Pluchino et al model Alex2013 (). The present results might be useful for examining such systems.

Acknowledgment

This work has been supported by TUBITAK (Turkish Agency) under the Research Project number 112T083. U.T. is a member of the Science Academy, Istanbul, Turkey. One of us (CT) acknowledges partial support from CNPq, Capes and Faperj (Brazilian agencies) and the John Templeton Foundation.

References

  • (1) S.H. Strogatz, Sync: The Emerging Science of Spontaneous Order (Hyperion, New York, 2004).
  • (2) A. Pikovski, M. Rosenblum and J. Kurths, Synchronization: A Universal Concept in Nonlinear Sciences (Cambridge University Press, Cambridge, 2001).
  • (3) K. Kaneko, Simulating Physics with Coupled Map Lattices (World Scientific, Singapore, 1990).
  • (4) T. Shibata, T. Chawanya and K. Kaneko, Phys. Rev. Lett. 82, 4424 (1999).
  • (5) J.N. Teramae and Y. Kuramoto, Phys. Rev. E 63, 036210 (2001).
  • (6) A. Pluchino, A. Rapisarda and C. Tsallis, Phys. Rev. E 87, 022910 (2013).
  • (7) M. De Menech and A.L. Stella, Physica A 309, 289 (2002).
  • (8) M.I. Bogachev and A. Bunde, Phys. Rev. E 78, 036114 (2008).
  • (9) J. Ludescher, C. Tsallis and A. Bunde, Europhys. Lett. 95, 68002 (2011).
  • (10) M.I. Bogachev, A.R. Kayumov and A. Bunde, PLoS ONE 9 (12), e112534 (2014).
  • (11) F. Caruso, A. Pluchino, V. Latora, S. Vinciguerra, and A. Rapisarda, Phys. Rev. E 75, 055101(R) (2007).
  • (12) B. Bakar and U. Tirnakli, Phys. Rev. E 79, 040103(R) (2009).
  • (13) B. Bakar and U. Tirnakli, Physica A 389, 3382 (2010).
  • (14) A. Celikoglu, U. Tirnakli and S.M.D. Queiros, Phys. Rev. E 82, 021124 (2010).
  • (15) C. Tsallis, Introduction to Nonextensive Statistical Mechanics: Approaching a Complex World (Springer, New York, 2009).
  • (16) S. Umarov, C. Tsallis and S. Steinberg, Milan J. Math. 76, 307 (2008); S. Umarov, C. Tsallis, M. Gell-Mann and S. Steinberg, J. Math. Phys. 51, 033502 (2010).
  • (17) U. Tirnakli and E.P. Borges, "The standard map: From Boltzmann-Gibbs statistics to Tsallis statistics", arXiv: 1501.02459, (2015).
Comments 0
Request Comment
You are adding the first comment!
How to quickly get a good reply:
  • Give credit where it’s due by listing out the positive aspects of a paper before getting into which changes should be made.
  • Be specific in your critique, and provide supporting evidence with appropriate references to substantiate general statements.
  • Your comment should inspire ideas to flow and help the author improves the paper.

The better we are at sharing our knowledge with each other, the faster we move forward.
""
The feedback must be of minimum 40 characters and the title a minimum of 5 characters
   
Add comment
Cancel
Loading ...
15811
This is a comment super asjknd jkasnjk adsnkj
Upvote
Downvote
""
The feedback must be of minumum 40 characters
The feedback must be of minumum 40 characters
Submit
Cancel

You are asking your first question!
How to quickly get a good answer:
  • Keep your question short and to the point
  • Check for grammar or spelling errors.
  • Phrase it like a question
Test
Test description