Non-Markovian Collective Motion from Self-Regulated Perceptual Dynamics
Pith reviewed 2026-05-18 03:13 UTC · model grok-4.3
The pith
Slow internal regulation in each agent generates non-Markovian collective motion through feedback from past alignments.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Each agent possesses a fast perceptual register encoding the tendency to align with neighbors and a slow regulatory variable that integrates recent alignment states before feeding this information back into alignment decisions. Using a positivity-preserving effective description for the internal states, the model produces non-Markovian collective motion when slow feedback operates, including slow-fast relaxation, feedback-induced hysteresis with finite memory-dependent loop area, and non-monotonic coordination between collective order and regulatory tone.
What carries the argument
The two-timescale model with a slow regulatory variable that integrates alignment history and provides feedback to alignment decisions.
If this is right
- The model exhibits slow-fast relaxation dynamics when the regulatory variable is active.
- Feedback induces hysteresis in the collective order parameter.
- The area of the hysteresis loop depends on the memory time scale.
- Coordination between collective order and regulatory tone is non-monotonic.
- In the fast-relaxation weak-feedback limit, it reduces to standard Vicsek alignment.
Where Pith is reading between the lines
- If real biological groups have similar internal regulatory processes, their collective motion should display history dependence even without explicit long-range interactions.
- Engineered swarms could be designed with tunable internal feedback to control memory and hysteresis in their behavior.
- Experimental tests could involve introducing controlled delays in agent responses and measuring resulting loop areas in order parameter plots.
Load-bearing premise
The slow regulatory variable integrates recent alignment states and feeds this back to alignment decisions in a manner that produces the reported non-Markovian signatures without further unstated rules.
What would settle it
If the hysteresis and memory-dependent loop areas disappear when the slow variable is removed or its integration time is set to zero, while other dynamics remain, that would confirm the role of the internal feedback.
Figures
read the original abstract
Collective motion in active matter is usually modelled through instantaneous local alignment, where each agent updates its heading from the current configuration of its neighbours. Many biological and engineered agents, however, possess internal regulatory variables that evolve more slowly than alignment itself and can store information about past alignment states. We introduce a minimal two-timescale model in which each agent carries a fast perceptual register and a slow regulatory variable. The fast register encodes the instantaneous tendency to align with neighbouring headings, while the slow variable integrates recent alignment and feeds back into subsequent alignment decisions. The internal dynamics are formulated using a GKSL-derived Bloch representation, used only as a positivity-preserving effective description of bounded two-state variables; no microscopic quantum dynamics is assumed. The model reduces to Vicsek-type alignment in the fast-relaxation, weak-feedback limit, but shows distinct behaviour when slow feedback is active. Simulations reveal slow-fast relaxation, feedback-induced hysteresis, finite memory-dependent loop area, and non-monotonic coordination between collective order and regulatory tone. These results show how effective non-Markovian collective motion can emerge from local internal feedback.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a minimal two-timescale model for collective motion in which each agent has a fast perceptual register encoding instantaneous alignment tendency and a slow regulatory variable that integrates recent alignment states and feeds back into alignment decisions. Internal dynamics use a GKSL-derived Bloch representation solely as a positivity-preserving effective description of bounded variables. The model reduces to Vicsek-type alignment in the fast-relaxation, weak-feedback limit but simulations show slow-fast relaxation, feedback-induced hysteresis with memory-dependent loop area, and non-monotonic coordination between collective order and regulatory tone, indicating emergence of effective non-Markovian collective motion from local internal feedback.
Significance. If the reported behaviors prove robust, the work would be significant for active matter by showing how internal regulatory variables can generate memory effects and non-Markovian signatures without explicit long-range or history terms, extending standard Vicsek models in a controlled way. The explicit reduction to Vicsek in the appropriate limit is a clear strength, as it is a direct consequence of the stated equations rather than a fitted outcome. The Bloch representation choice for effective bounded dynamics is a reasonable modeling device.
major comments (2)
- Abstract, paragraph describing the two-timescale model: the central claim that the slow regulatory variable's integration of recent alignment states plus feedback produces effective non-Markovian signatures (hysteresis, finite memory-dependent loop area, non-monotonic order-regulatory coordination) requires the precise update rules, coupling function, and normalizations in the GKSL-derived Bloch map to be specified; without them it is unclear whether these behaviors are generic to local internal feedback or artifacts of particular implementation choices.
- Simulations section: the reported outcomes for hysteresis and non-monotonic coordination provide no quantitative error bars, parameter tables, or explicit checks that the behaviors survive changes in integration rules or neighbor definitions, which is necessary to support that they constitute distinct behaviour beyond the Vicsek limit.
minor comments (2)
- The free parameters (timescale separation ratio and feedback coupling strength) should be listed with their ranges and default values in a dedicated table to aid reproducibility.
- Clarify in the model section whether the Bloch representation introduces any additional normalizations beyond positivity preservation, and how these affect the feedback mapping.
Simulated Author's Rebuttal
We are grateful to the referee for the positive assessment of the work's significance and for the detailed comments that will help improve the manuscript. We address the major comments point by point below, indicating the revisions we plan to implement.
read point-by-point responses
-
Referee: Abstract, paragraph describing the two-timescale model: the central claim that the slow regulatory variable's integration of recent alignment states plus feedback produces effective non-Markovian signatures (hysteresis, finite memory-dependent loop area, non-monotonic order-regulatory coordination) requires the precise update rules, coupling function, and normalizations in the GKSL-derived Bloch map to be specified; without them it is unclear whether these behaviors are generic to local internal feedback or artifacts of particular implementation choices.
Authors: We agree that the abstract, being a concise summary, does not include the full mathematical details. However, the manuscript's Section II provides the explicit update rules for the fast perceptual register (using the Bloch vector representation derived from the GKSL equation) and the slow regulatory variable, including the coupling function f(·) and normalization constants that ensure positivity and boundedness. To make this clearer in the abstract, we will revise it to briefly state that the internal dynamics follow a positivity-preserving Bloch map with specific relaxation rates and feedback strength, and we will add a sentence noting that the non-Markovian effects arise generically from the separation of timescales and the feedback loop, as confirmed by the reduction to the Vicsek model in the appropriate limit. This revision will be made. revision: yes
-
Referee: Simulations section: the reported outcomes for hysteresis and non-monotonic coordination provide no quantitative error bars, parameter tables, or explicit checks that the behaviors survive changes in integration rules or neighbor definitions, which is necessary to support that they constitute distinct behaviour beyond the Vicsek limit.
Authors: The referee is correct that the current version of the simulations section lacks error bars and robustness checks. We will revise the manuscript to include: (i) error bars computed from 10 independent runs with different random seeds for each parameter set; (ii) a table listing all key parameters (e.g., alignment strength, feedback rate, relaxation times, system size, density); (iii) additional figures or text demonstrating that the hysteresis loops and non-monotonic coordination persist under variations in the numerical integration scheme (e.g., Euler vs. Runge-Kutta) and neighbor definitions (metric distance vs. fixed number of nearest neighbors). These additions will confirm that the observed non-Markovian signatures are robust features of the model rather than numerical artifacts. revision: yes
Circularity Check
Derivation self-contained: explicit rules yield emergent signatures without reduction to inputs
full rationale
The paper defines a two-timescale model via explicit dynamical equations for the fast perceptual register and slow regulatory variable, using a GKSL-derived Bloch map solely as a positivity-preserving effective description. The reduction to Vicsek alignment is stated as a direct mathematical limit of those equations in the fast-relaxation weak-feedback regime. Reported behaviors (hysteresis, memory-dependent loop area, non-monotonic coordination) are obtained from numerical integration of the stated update rules rather than from any fitted parameter or self-referential prediction. No self-citations are invoked as load-bearing uniqueness theorems, and no ansatz is smuggled via prior work. The central claim therefore rests on the independent content of the model equations and their simulation outputs, not on any circular re-expression of the inputs.
Axiom & Free-Parameter Ledger
free parameters (2)
- timescale separation ratio
- feedback coupling strength
axioms (1)
- domain assumption The internal state dynamics admit a positivity-preserving Bloch representation derived from GKSL form, used solely as an effective description of bounded two-state variables.
invented entities (1)
-
slow regulatory variable
no independent evidence
Reference graph
Works this paper leans on
-
[1]
Princeton University Press, 2010
David JT Sumpter.Collective animal behavior. Princeton University Press, 2010
work page 2010
-
[2]
Collective motion.Physics reports, 517(3-4):71–140, 2012
Tam ´as Vicsek and Anna Zafeiris. Collective motion.Physics reports, 517(3-4):71–140, 2012
work page 2012
-
[3]
The physics of life.Nature, 529(7584):16, 2016
Gabriel Popkin. The physics of life.Nature, 529(7584):16, 2016
work page 2016
-
[4]
Michele Ballerini, Nicola Cabibbo, Raphael Candelier, Andrea Cavagna, Evaristo Cis- bani, Irene Giardina, Vivien Lecomte, Alberto Orlandi, Giorgio Parisi, Andrea Procac- cini, et al. Interaction ruling animal collective behavior depends on topological rather than metric distance: Evidence from a field study.Proceedings of the national academy of sciences,...
work page 2008
-
[5]
Sara Brin Rosenthal, Colin R Twomey, Andrew T Hartnett, Hai Shan Wu, and Iain D Couzin. Revealing the hidden networks of interaction in mobile animal groups allows prediction of complex behavioral contagion.Proceedings of the National Academy of Sciences, 112(15):4690–4695, 2015
work page 2015
-
[6]
Yi Ma, Eric Wai Ming Lee, Meng Shi, and Richard Kwok Kit Yuen. Spontaneous synchro- nization of motion in pedestrian crowds of different densities.Nature human behaviour, 5(4):447–457, 2021
work page 2021
-
[7]
Yann-Edwin Keta, Robert L Jack, and Ludovic Berthier. Disordered collective motion in dense assemblies of persistent particles.Physical Review Letters, 129(4):048002, 2022
work page 2022
-
[8]
Emergent complex neural dynamics.Nature physics, 6(10):744–750, 2010
Dante R Chialvo. Emergent complex neural dynamics.Nature physics, 6(10):744–750, 2010
work page 2010
-
[9]
Haitao Zhao, Hai Liu, Yiu-Wing Leung, and Xiaowen Chu. Self-adaptive collective motion of swarm robots.IEEE Transactions on Automation Science and Engineering, 15(4):1533–1545, 2018
work page 2018
-
[10]
Tam ´as Vicsek, Andr´as Czir ´ok, Eshel Ben-Jacob, Inon Cohen, and Ofer Shochet. Novel type of phase transition in a system of self-driven particles.Physical review letters, 75(6):1226, 1995. 14
work page 1995
-
[11]
Flocks, herds, and schools: A quantitative theory of flocking
John Toner and Yuhai Tu. Flocks, herds, and schools: A quantitative theory of flocking. Physical review E, 58(4):4828, 1998
work page 1998
-
[12]
John J Hopfield. Neural networks and physical systems with emergent collective com- putational abilities.Proceedings of the national academy of sciences, 79(8):2554–2558, 1982
work page 1982
-
[13]
Quantum-like modeling of cognition.Frontiers in Physics, 3:77, 2015
Andrei Khrennikov. Quantum-like modeling of cognition.Frontiers in Physics, 3:77, 2015
work page 2015
-
[14]
Aghdas Meghdadi, Mohammad-R Akbarzadeh-T, and Kurosh Javidan. A quantum-like model for predicting human decisions in the entangled social systems.IEEE Transactions on Cybernetics, 52(7):5778–5788, 2022
work page 2022
-
[15]
A quantum probability account of order effects in inference.Cognitive science, 35(8):1518–1552, 2011
Jennifer S Trueblood and Jerome R Busemeyer. A quantum probability account of order effects in inference.Cognitive science, 35(8):1518–1552, 2011
work page 2011
-
[16]
Andrei Khrennikov and Irina Basieva. Entanglement of observables: quantum conditional probability approach.F oundations of Physics, 53(5):84, 2023
work page 2023
-
[17]
Peter D Bruza, Zheng Wang, and Jerome R Busemeyer. Quantum cognition: a new theoretical approach to psychology.Trends in cognitive sciences, 19(7):383–393, 2015
work page 2015
-
[18]
Jan Broekaert, Irina Basieva, Pawel Blasiak, and Emmanuel M Pothos. Quantum-like dynamics applied to cognition: a consideration of available options.Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences, 375(2106):20160387, 2017
work page 2017
-
[19]
Jyotiranjan Beuria, Mayank Chaurasiya, and Laxmidhar Behera. Collective motion from quantum-inspired dynamics in visual perception.Proceedings of the Royal Society A, 481(2321):20250489, 2025
work page 2025
-
[20]
Stuart Hameroff and Roger Penrose. Consciousness in the universe: A review of the ‘orch or’theory.Physics of life reviews, 11(1):39–78, 2014
work page 2014
-
[21]
Fabio Bagarello, Irina Basieva, and Andrei Khrennikov. Quantum field inspired model of decision making: Asymptotic stabilization of belief state via interaction with surrounding mental environment.Journal of Mathematical Psychology, 82:159–168, 2018
work page 2018
-
[22]
Andrei Y Khrennikov.Open quantum systems in biology, cognitive and social sciences. Springer Nature, 2023
work page 2023
-
[23]
Shaun Gallagher. Philosophical conceptions of the self: implications for cognitive sci- ence.Trends in cognitive sciences, 4(1):14–21, 2000
work page 2000
-
[24]
The multisensory basis of the self: From body to identity to others
Manos Tsakiris. The multisensory basis of the self: From body to identity to others. Quarterly journal of experimental psychology, 70(4):597–609, 2017
work page 2017
-
[25]
Cortical midline structures and the self.Trends in cognitive sciences, 8(3):102–107, 2004
Georg Northoff and Felix Bermpohl. Cortical midline structures and the self.Trends in cognitive sciences, 8(3):102–107, 2004. 15
work page 2004
-
[26]
F Schneider, Felix Bermpohl, A Heinzel, Michael Rotte, Martin Walter, C Tempelmann, Christina Wiebking, Henrik Dobrowolny, HJ Heinze, and Georg Northoff. The resting brain and our self: self-relatedness modulates resting state neural activity in cortical mid- line structures.Neuroscience, 157(1):120–131, 2008
work page 2008
-
[27]
Pengmin Qin and Georg Northoff. How is our self related to midline regions and the default-mode network?Neuroimage, 57(3):1221–1233, 2011
work page 2011
-
[28]
Mapping the self in the brain’s default mode network.NeuroImage, 132:390–397, 2016
Christopher G Davey, Jesus Pujol, and Ben J Harrison. Mapping the self in the brain’s default mode network.NeuroImage, 132:390–397, 2016
work page 2016
-
[29]
Peter Fransson. Spontaneous low-frequency bold signal fluctuations: An fmri investiga- tion of the resting-state default mode of brain function hypothesis.Human brain mapping, 26(1):15–29, 2005
work page 2005
-
[30]
Vittorio Gorini, Andrzej Kossakowski, and Ennackal Chandy George Sudarshan. Com- pletely positive dynamical semigroups of n-level systems.Journal of Mathematical Physics, 17(5):821–825, 1976
work page 1976
-
[31]
Goran Lindblad. On the generators of quantum dynamical semigroups.Communications in mathematical physics, 48(2):119–130, 1976
work page 1976
-
[32]
Caspar M Schwiedrzik, Christian C Ruff, Andreea Lazar, Frauke C Leitner, Wolf Singer, and Lucia Melloni. Untangling perceptual memory: Hysteresis and adaptation map into separate cortical networks.Cerebral Cortex, 24(5):1152–1164, 2014
work page 2014
-
[33]
Sonia Poltoratski and Frank Tong. Hysteresis in the dynamic perception of scenes and objects.Journal of Experimental Psychology: General, 143(5):1875, 2014
work page 2014
-
[34]
Hysteresis in audiovisual synchrony perception.PloS one, 10(3):e0119365, 2015
Jean-Remy Martin, Anne K ¨osem, and Virginie van Wassenhove. Hysteresis in audiovisual synchrony perception.PloS one, 10(3):e0119365, 2015. 16
work page 2015
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.