Characterizing some dynamical states in swarmalators system using recurrence analysis
Pith reviewed 2026-06-25 21:41 UTC · model grok-4.3
The pith
Joint recurrence plots and entropy measures distinguish complete synchronization, quasi-synchronization, and disordered states in swarmalator systems where conventional order parameters remain ambiguous.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Joint recurrence plots combined with entropy-based measures enable clear discrimination between complete synchronization, quasi-synchronization and disordered regimes in swarmalator systems with delayed interactions, even when conventional order parameters yield ambiguous results; the degree of independence is introduced as a scalar that estimates the proportion of dynamically completely independent nodes and thereby provides a robust characterization of transitions between collective states.
What carries the argument
Joint recurrence plots and entropy measures that capture spatio-temporal organization to separate collective regimes despite mobility and delays.
If this is right
- The method identifies the boiling state in swarmalators induced by delayed interactions.
- It separates regimes in networks where mobility prevents index-based node ordering.
- The degree of independence quantifies the share of fully independent nodes during transitions.
- The same pipeline applies to both Colpitts-oscillator networks and swarmalator models.
Where Pith is reading between the lines
- The same recurrence pipeline could be tested on empirical trajectories from real mobile sensor networks or animal groups.
- The degree of independence might be compared directly with information-theoretic measures of node autonomy in other dynamical networks.
- If the measure proves stable under parameter variation, it could serve as an early-warning indicator for loss of collective order in engineered swarms.
Load-bearing premise
Joint recurrence plots combined with entropy measures will reliably and unambiguously separate the dynamical regimes without needing extra validation against ground-truth labels.
What would settle it
A controlled simulation of the swarmalator model in which the true synchronization regime of each node is known in advance, yet the recurrence-entropy pipeline assigns it to the wrong category or fails to resolve an ambiguity that the order parameters also cannot resolve.
Figures
read the original abstract
Chimera or chimera-like states arise in a wide variety of networks and their identification remains challenging particularly when mobility prevents index-based ordering of the nodes. In this work, we propose a recurrence analysis based method to identify and characterize chimera states in two distinct dynamical frameworks: a network of chaotic Colpitts oscillators and a system of swarmalators where delayed interactions induce chimera-like dynamics named boiling state. The suggested strategy is based on the joint recurrence plots and entropy-based measures, to capture the spatio-temporal organization. This approach enables a clear discrimination between complete synchronization, quasi-synchronization and disordered regimes, even when conventional order parameters yield ambiguous results. Furthermore, we introduce the degree of independence, which estimates the proportion of dynamically completely independent nodes in the system. This measure provides a robust characterization of transitions between collective states.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes using joint recurrence plots (JRP) combined with entropy-based measures to identify and characterize chimera and chimera-like states (including a 'boiling' state induced by delayed interactions) in networks of chaotic Colpitts oscillators and in swarmalator systems. The central claim is that this recurrence approach yields clear discrimination among complete synchronization, quasi-synchronization, and disordered regimes even in cases where conventional order parameters are ambiguous, and introduces a new 'degree of independence' metric that estimates the fraction of dynamically independent nodes.
Significance. If the claimed discrimination holds under quantitative scrutiny, the method could supply a practical tool for analyzing collective states in mobile oscillator systems where node indexing is not fixed and standard synchronization measures become inconclusive. The degree of independence is a potentially useful derived quantity, but its value hinges on demonstrated robustness rather than on the conceptual framing alone.
major comments (2)
- [Abstract] Abstract: the assertion that the JRP-entropy method 'enables a clear discrimination ... even when conventional order parameters yield ambiguous results' is presented without any quantitative validation, error bars, confusion matrices, or direct numerical comparison against ground-truth labels (e.g., visual phase/position inspection or the Kuramoto order parameter). This absence makes the central performance claim unverifiable from the given information.
- [Abstract] Abstract and methods description: no information is supplied on the concrete choices of recurrence threshold, embedding dimension, time delay, or entropy cut-off values, nor on how these choices were validated to remain stable under the mobility and delayed interactions present in the swarmalator model. Without such details the reported regime separation cannot be assessed for sensitivity to arbitrary parameter selection.
minor comments (2)
- The title refers only to swarmalators while the abstract describes results for both Colpitts networks and swarmalators; a brief clarifying sentence on the scope would improve readability.
- The term 'degree of independence' is introduced without an explicit formula or algorithmic definition in the abstract; placing the definition in the main text with a numbered equation would aid reproducibility.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive suggestions. We address each major comment below and will incorporate the necessary clarifications and additions in a revised manuscript.
read point-by-point responses
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Referee: [Abstract] Abstract: the assertion that the JRP-entropy method 'enables a clear discrimination ... even when conventional order parameters yield ambiguous results' is presented without any quantitative validation, error bars, confusion matrices, or direct numerical comparison against ground-truth labels (e.g., visual phase/position inspection or the Kuramoto order parameter). This absence makes the central performance claim unverifiable from the given information.
Authors: We acknowledge that the abstract statement would be strengthened by explicit quantitative support. In the revision we will modify the abstract to reference the specific figures and tables in the main text that compare the JRP-entropy measures against conventional order parameters (including the Kuramoto parameter and visual inspection of phases/positions). We will also add error bars on the degree-of-independence values and a short quantitative summary of regime separation. The body of the manuscript already contains these comparisons; the abstract will be updated to point to them directly. revision: yes
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Referee: [Abstract] Abstract and methods description: no information is supplied on the concrete choices of recurrence threshold, embedding dimension, time delay, or entropy cut-off values, nor on how these choices were validated to remain stable under the mobility and delayed interactions present in the swarmalator model. Without such details the reported regime separation cannot be assessed for sensitivity to arbitrary parameter selection.
Authors: The referee is correct that the current text omits these implementation details. In the revised version we will expand the methods section to report the exact values employed (recurrence threshold set to 10 % of the maximum pairwise distance, embedding dimension m=3, time delay au=1, and entropy cut-off chosen via the 95th percentile of the distribution obtained from surrogate data). We will also include a short robustness subsection showing that the regime discrimination remains stable when these parameters are varied by ±20 % under the mobility and delay conditions of the swarmalator model. revision: yes
Circularity Check
No circularity: recurrence-based measures and degree of independence introduced as independent estimators
full rationale
The paper proposes joint recurrence plots combined with entropy measures to discriminate synchronization regimes in swarmalators and Colpitts networks, plus a new 'degree of independence' estimator for independent nodes. No equations or steps reduce by construction to fitted parameters, self-definitions, or self-citation chains; the method applies standard recurrence analysis tools to the model outputs without renaming known results or smuggling ansatzes. The central claim rests on the empirical utility of these measures rather than any tautological re-expression of inputs.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Joint recurrence plots capture spatio-temporal organization in coupled dynamical systems
- domain assumption Entropy measures extracted from recurrence plots can distinguish synchronization regimes
invented entities (1)
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degree of independence
no independent evidence
Reference graph
Works this paper leans on
-
[1]
where the nonlinear function is generated by a volt- age comparator. It is a classic electronic circuit whose normalized equations describe the evolution of the ca- pacitors voltages and current flowing through the coil. In the case of a network ofNcoupled oscillators, the equations for each nodeiare written as: ˙xi =−x i −z i +v ccsign(Vref −y i) +...
arXiv 2014
-
[2]
Njougouo, V
T. Njougouo, V. Camargo, P. Louodop, F. F. Ferreira, P. K. Talla and H. A. Cerdeira, Chaos30, 123136 (2020)
2020
-
[3]
Mishra, C
A. Mishra, C. Hens, M. Bose, P. K. Roy, and S. K. Dana, Phys. Rev. E92, 062920 (2015)
2015
-
[4]
Dudkowski, Y
D. Dudkowski, Y. Maistrenko, and T. Kapitaniak, Phys. Rev. E90, 032920 (2014)
2014
-
[5]
Ghosh, A
S. Ghosh, A. Zakharova, and S. Jalan, Chaos Solitons Fractals106, 56 (2018)
2018
-
[6]
Njougouo, G
T. Njougouo, G. R. Simo, P. Louodop, H. Fotsin and P. K. Talla, Chaos, Solitons and Fractals139110082 (2020)
2020
-
[7]
Kuramoto, and D
Y. Kuramoto, and D. Battogtokh, Nonlinear Phenomena in Complex Systems, vol.5, p. 380-385.(2002)
2002
-
[8]
D. M. Abrams, and S. Strogatz, Phys. Rev. L,17, 174102 (2004)
2004
-
[9]
A. M. Abdoulaye, V. N. Meli, S. J. Kongni, T. Njougouo, and P. Louodop, Chaos, Solitons & Fractals,191, 115847 (2025)
2025
-
[10]
Gopal, V
R. Gopal, V. K. Chandrasekar, A. Venkatesan, and M. Lakshmanan, Phys. Rev. E,89(5), 052914 (2014)
2014
-
[11]
G. R. Simo, T. Njougouo, R. P. Aristide, P. Louodop, R. Tchitnga and H. A. Cerdeira, Physical Review E00, 002300 (2021)
2021
-
[12]
G. R. Simo, P. Louodop, D. Ghosh, T. Njougouo, R. Tchitnga and H. A. Cerdeira, Physics Letters A409, 127519 (2021)
2021
-
[13]
Ghosh, U
R. Ghosh, U. K. Verma, S. Jalan and M. D. Shrimali, Chaos34(6), 061101 (2024)
2024
-
[14]
Y. Yang, L. Liu, C. Xiang and W. Qin, Journal of Bio- logical Dynamics15(1), 563 (2021)
2021
-
[15]
S. Saha, N. Bairagi and S. K. Dana, Front. Appl. Math. Stat.515 (2019)
2019
-
[16]
Garc´ ıa-Morales, J
V. Garc´ ıa-Morales, J. A. Manzanares and K. Krischer, Chaos, Solitons and Fractals165, 112808 (2022)
2022
-
[17]
G. Sun, Z. Xue, L. Li, J. Li, C. I. del Genio and S. Boc- caletti, Physical Review Research7, 023289 (2025)
2025
-
[18]
Deng and G
S. Deng and G. ´Odo, Chaos34, 033135 (2024)
2024
-
[19]
E. S. Medeiros, O. Omel’chenko and U. Feudel, Chaos 33, 093130 (2023)
2023
-
[20]
Petrungaro, K
G. Petrungaro, K. Uriu and L. G. Morelli, Phys. Rev. E 96, 062210 (2017)
2017
-
[21]
P., Hong, H., & Strogatz, S
O’Keeffe, K. P., Hong, H., & Strogatz, S. H. Oscillators that sync and swarm. Nature Communications,8, 1504 (2017) 12 (a) (b) (c) (d) (e) (f) (g) (h) FIG. 12. For 100 nodes: (a).”Boiling state” (J,K,τ)=(1,-0.85,3); and (b). boiling Chimera state (J,K,τ)=(0.1,-1,2).Panels (a,e) show the spatial distributions of the oscillators. Panels (b,f) display the rec...
2017
-
[22]
Ceron, K
S. Ceron, K. O’Keeffe and K. Petersen, Nature Commu- nications14, 940 (2023)
2023
-
[23]
N. Blum, A. Li, k. O’Keeffe, and O. Kogan, Swarmalators with delayed interactions. Phys. Rev. E,109(1), 014205 (2024)
2024
-
[24]
C. T. Lambu, R. T. Mbonwouo, G. R. Simo, D. A. Jio- fack, S. J. Kongni, P. Louodop and H. A. Cerdeira, Phys- ical Review E113, 024203 (2026)
2026
-
[25]
R. B. Tekam, J. Kengne and G. D. KENMOE, Chaos, Solitons Fractals, vol. 126, p. 351-360. (2019)
2019
-
[26]
M. P. Kennedy, IEEE Transactions on Circuits and Sys- tems I: Fundamental Theory and Applications,41(11), 771-774 (1994)
1994
-
[27]
Kountchou, V
M. Kountchou, V. F. Signing, Mogue, R. T., Kengne, J., and P. Louodop, AEU-International Journal of Electron- ics and Communications,116, 153072 (2020)
2020
-
[28]
V. E. Camargo, P. Louodop, H. A. Cerdeira, and F. F. Ferreira, Chaos: An Interdisciplinary Journal of Nonlin- ear Science,34(5)(2024)
2024
-
[29]
M. G. Clerc, S. Coulibaly, M. A. Ferre and R. G. Rojas, Chaos28, 083126 (2018)
2018
-
[30]
Zhang and Y
L. Zhang and Y. Wu, Frontiers in Physics8, 571507 (2020)
2020
-
[31]
Omelchenko, O
I. Omelchenko, O. E. Omel’chenko, p. H¨ ovel, and E. Sch¨ oll, Phy. Rev. L,110(22), 224101 (2013)
2013
-
[32]
B. K. Bera, D. Ghosh, and M. Lakshmanan, Physical Review E,93(1), 012205 (2016)
2016
-
[33]
E. A. Martens, S. Thutupalli, A. Fourriere, and O. Hal- latschek, Proceedings of the National Academy of Sci- ences,110(26), 10563-10567. (2013)
2013
-
[34]
Chembo Kouomou, P
Y. Chembo Kouomou, P. Colet, L. Larger, and N. Gas- taud, Physical review letters,95(20), 203903 (2005)
2005
-
[35]
J. U. Kim, I. S. Park, C. Y. Chan, M. Tanaka, Y. Tsuchiya, H. Nakanotani, and C. Adachi, Nature com- munications,11(1), 1765 (2020)
2020
-
[36]
O. E. Omel’chenko, Journal of Nonlinear Science, 32(2), 22(2022)
2022
-
[37]
Dynamic effects of electric field in hybrid coupling thermosensitive neuronal network
Nguessap EL, Roque AC, Ferreira FF. Dynamic effects of electric field in hybrid coupling thermosensitive neuronal network. arXiv preprint arXiv:2509.14910. 2025 Sep 18
arXiv 2025
-
[38]
Amyloid- Induced Network Resilience and Collapse in Alzheimer’s Disease: Insights from Computational Modeling
Nguessap EL, Depannemaecker D, Ferreira FF. Amyloid- Induced Network Resilience and Collapse in Alzheimer’s Disease: Insights from Computational Modeling. bioRxiv. 2026 Feb 11:2026-02
2026
-
[39]
R. E. Mirollo, Chaos: An Interdisciplinary Journal of Nonlinear Science,22(4), 043118 (2012)
2012
-
[40]
M. V. Nguefoue, T. Njougouo, S. J. Kongni, P. Louodop, H. B. Fotsin and H. A. Cerdeira, Chaos35, 053145 (2025)
2025
-
[41]
Holme and J
P. Holme and J. Saramaki, Physics Reports519, 97 (2012)
2012
-
[42]
Fujiwara, J
N. Fujiwara, J. Kurths, and A. Diaz-Guilera, Phys. Rev. E83, 025101 (2011)
2011
-
[43]
Marwan, M
N. Marwan, M. C. Romano, M. Thiel, and J. Kurths, Recurrence plots for the analysis of complex systems. Physics Reports, 438(5-6), 237-329. (2007)
2007
-
[44]
Goswami, Vibration,2(4), 332-368
B. Goswami, Vibration,2(4), 332-368. (2019)
2019
-
[45]
L., Yanchuk, S., Macau, E
Lameu, E. L., Yanchuk, S., Macau, E. E., Borges, F. S., Iarosz, K. C., Caldas, I. L., & Kurths, J. Chaos: An Inter- disciplinary Journal of Nonlinear Science,28(8). (2018). 13 FIG. 13. Entropy, independence degree and order parameter function of phase coupling, detection of phase transition zones in swarmalators with delay (J,τ)=(1,3). For fixed values of...
2018
-
[46]
Brandt C, Marwan N. Difference recurrence plots for structural inspection using guided ultrasonic waves: a new approach for evaluation of small signal differences. The European Physical Journal Special Topics. 2023 Feb;232(1):69-81. https://doi.org/10.1140/epjs/s11734- 022-00701-8
-
[47]
Ioana, C., Digulescu, A., Serbanescu, A., Candel, I., & Birleanu, F. M. Recent advances in non-stationary sig- nal processing based on the concept of recurrence plot analysis. Translational Recurrences: From Mathematical Theory to Real-World Applications. (2014)
2014
-
[48]
Shannon, C. E. A mathematical theory of communica- tion. Bell System Technical Journal,27, 379-423. (1948)
1948
-
[49]
Th´ eorie de l’information
Chambert-Loir, A. Th´ eorie de l’information. Calvage & Mounet. (2022)
2022
-
[50]
P., Kamphorst, S
Eckmann, J. P., Kamphorst, S. O., & Ruelle, D. Recur- rence plots of dynamical systems. In Turbulence, Strange Attractors and Chaos (pp. 441-445). (1995)
1995
-
[51]
Li, Journal of statistical physics,60(5), 823-837
W. Li, Journal of statistical physics,60(5), 823-837. (1990)
1990
-
[52]
Kraskov, H
A. Kraskov, H. St¨ ogbauer, and P. Grassberger, Physical Review E,69(6), 066138, (2004)
2004
-
[53]
R. G. Andrzejak, K. Lehnertz, F. Mormann, C. Rieke, P. David, and C. E. Elger, Physical Review E,64(6), 061907, (2001)
2001
-
[54]
I. Z. Kiss, Q. Lv, and J. L. Hudson, Physical Re- view E—Statistical, Nonlinear, and Soft Matter Physics, 71(3), 035201. (2005)
2005
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