The paper [1] gives the concept of multidimensional map aswith and f is generated from the gene scalar functionwith .
The multidimensional logistic map is therefore given byas defined in [2].
In [1] the discussion is oriented to the invariance of the bifurcation diagrams of the multidimensional maps with respect to that of the corresponding gene scalar map, not limiting to the logistic map case. We remark that in [1] the interest is towards ensuring as a first condition the non-explosivity of the multidimensional map, therefore the aim of Theorems 1 and 2 in [1] is to determine the conditions under which non-explosivity is guaranteed. Theorems 1 and 2, in fact, guarantee that the multidimensional maps are not explosive if the eigenvalues of the diagonalizable initial condition matrix are inside the basin of attraction of the corresponding scalar map.
In the Commentary [3], an example on the multidimensional logistic map is reported with the aim of invalidating the theory presented in [1]. It assumed as initial condition the matrix with eigenvalues λ1 = λ2 = 0.1. The authors show the explositivity of the map by using a numerical simulation.
Fact. The example does not match the assumptions of Theorem 1. In fact, the assumed matrix X(0) is not diagonalizable. In the proof of Theorem 1 [1], Eq. 9 is immediately followed by the sentence: “with X(0) = TXD(0)T−1 being XD(0) a diagonal matrix containing the eigenvalues of X(0) and the matrix of eigenvectors.” The proof is performed under this hypothesis. Therefore, even if the eigenvalues of the considered X(0) are in basin of attraction of the scalar logistic map, it is verified that it is not diagonalizable being X(0) a 2 × 2 not diagonal matrix with identical eigenvalues. For this matrix a Jordan form can be derived aswith and being J a not diagonal matrix and thus not respecting the assumptions of Theorem 1.
Moreover, in the case of with n > 2 admitting eigenvalues with multiplicity greater than 1, the theory does hold if X(0) is diagonalizable. As an example, let us consider as initial condition the matrix . This matrix admits two identical eigenvalues λ1 = λ2 = 0.1 and a third eigenvalue λ3 = 0.2. Matrix X(0) is symmetrical and hence diagonalizable, and all eigenvalues are in the basin of attraction of the scalar logistic map. The multidimensional logistic map is, in fact, not explosive, as guaranteed by Theorems 1 and 2.
The authors of [3] chose a not correct example to put in crisis the validity of paper [1].
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Author contributions
All authors listed have made a substantial, direct, and intellectual contribution to the work and approved it for publication.
Funding
This work has been partially funded by European Union (Next-Generation EU), through the MUR-PNRR project “FAIR: Future Artificial Intelligence Research” (E63C22001940006). This work has been partially carried out within the framework of the EUROfusion Consortium, funded by the European Union via the Euratom Research and Training Programme (Grant Agreement No. 101052200—EUROfusion). Views and opinions expressed are however those of the author(s) only and do not necessarily reflect those of the European Union or the European Commission. Neither the European Union nor the European Commission can be held responsible for them.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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References
1.
BucoloMBuscarinoAFortunaLGaglianoS. Multidimensional discrete chaotic maps. Front Phys (2022) 199. 10.3389/fphy.2022.862376
2.
NavickasZSmidtaiteRVainorasARagulskisM. The logistic map of matrices. Discrete & Continuous Dynamical Systems-B (2011) 16:927–44. 10.3934/dcdsb.2011.16.927
3.
SmidtaiteRRagulskisM. Commentary: Multidimensional discrete chaotic maps. Front. Phys. (2022) 10:1094240.
Summary
Keywords
nonlinear dyanamics, discrete map, bifurcation, chaos, multidimensional systems
Citation
Bucolo M, Buscarino A, Fortuna L and Gagliano S (2023) Response to: Commentary: Multidimensional discrete chaotic maps. Front. Phys. 11:1134524. doi: 10.3389/fphy.2023.1134524
Received
30 December 2022
Accepted
23 January 2023
Published
13 February 2023
Volume
11 - 2023
Edited by
Riccardo Meucci, Department of Physical Sciences and Technologies of Matter (CNR), Italy
Reviewed by
Sajad Jafari, Amirkabir University of Technology, Iran
Jean-Marc Ginoux, Université de Toulon, France
Updates
Copyright
© 2023 Bucolo, Buscarino, Fortuna and Gagliano.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Luigi Fortuna, luigi.fortuna@unict.it
This article was submitted to Interdisciplinary Physics, a section of the journal Frontiers in Physics
Disclaimer
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article or claim that may be made by its manufacturer is not guaranteed or endorsed by the publisher.