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arxiv: 2601.13595 · v2 · pith:5GTLC4BYnew · submitted 2026-01-20 · ❄️ cond-mat.stat-mech

Macroscopic localization and collective memory in Poisson renewal resetting

Pith reviewed 2026-05-21 16:35 UTC · model grok-4.3

classification ❄️ cond-mat.stat-mech
keywords renewal processesPoissonian resetscollective memorydynamical phase transitionlocalizationaging dynamicscontinuous-time random walksecological organization
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0 comments X

The pith

Ensembles of continuous-time random walkers with Poissonian resets develop macroscopic localization at the reset point and undergo a discontinuous transition to collective memory under interactions.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper shows that stochastic renewal processes with Poissonian resets on continuous-time random walkers produce a mixed discrete-continuous structure, where a macroscopic fraction of particles localize at the reset configuration. An age-structured framework demonstrates this localization effect from the renewal dynamics. Collective interactions allow the system to retain memory of past states even though every individual reset event is memoryless. This produces a discontinuous dynamical phase transition from weak collective bias with stationary dynamics to strong collective bias with nonstationary aging dynamics up to finite-size effects. A reader would care because the result supplies a concrete mechanism for how macroscopic structure and long-term collective memory can arise in stochastic systems from rules that lack memory at the single-particle level, with explicit ecological implications.

Core claim

For ensembles of continuous-time random walkers subject to Poissonian renewal resets, the discrete component corresponds to localization at the reset configuration. Collective interactions can retain memory although all reset events are memoryless. The transition to collective memory is discontinuous, and the model identifies a discontinuous dynamical phase transition from weak collective bias, where the dynamics are stationary, to strong collective bias where the dynamics are nonstationary and display aging up to finite-size effects.

What carries the argument

Age-structured framework for Poissonian renewal resetting, which decomposes the particle distribution into discrete and continuous components and tracks how collective bias couples to the age structure.

If this is right

  • A macroscopic fraction of walkers occupies the discrete localized state at the reset configuration.
  • Collective interactions enable retention of memory despite memoryless individual resets.
  • The transition from stationary to aging nonstationary dynamics occurs discontinuously as collective bias strengthens.
  • These mechanisms shape macroscopic structure and collective organization in ecological systems.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • This supplies a general route by which memoryless stochastic rules at the individual level can produce effective long-term memory at the population scale.
  • Analogous localization and abrupt memory transitions may appear in other renewal-driven systems such as queuing networks or signaling cascades.
  • Finite-size scaling of the aging regime could be tested by varying system size in simulations to locate the boundary between weak and strong bias.

Load-bearing premise

Reset events remain strictly Poissonian and memoryless even when collective interactions are present, and the age-structured framework fully captures the mixed discrete-continuous structure without additional spatial or interaction details.

What would settle it

A direct measurement or simulation of the fraction of particles in the localized discrete state as reset rate and interaction strength vary, or a plot of the order parameter for stationarity versus aging that shows a jump rather than a smooth crossover.

Figures

Figures reproduced from arXiv: 2601.13595 by Ohad Vilk.

Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: summarizes these results for β = 0.8, illustrat￾ing aging of the condensation m(t) for 1 ≪ t < tc [4(a)] and the scaling of a finite-size cutoff time tc with N [4(b)]. We further show that at fixed time, the dynamical transi￾tion sharpens and approaches ζ = 1 as N increases [4(c)]. Finally, for ζ < 1 or t > tc the dynamics are stationary with γ ≃ 0, while for ζ > 1 and t < tc we have a sharp transition to … view at source ↗
read the original abstract

Stochastic renewal processes are ubiquitous across physics, biology, and the social sciences. Here, we show that continuous-time renewal dynamics can naturally produce a mixed discrete-continuous structure, with a macroscopic fraction of particles occupying a discrete state. For ensembles of continuous-time random walkers subject to Poissonian renewal resets, we develop an age-structured framework showing this discrete component corresponds to localization at the reset configuration. We next show that collective interactions can retain memory although all reset events are memoryless. Remarkably, the transition to collective memory is discontinuous, and we identify a discontinuous dynamical phase transition from weak collective bias, where the dynamics are stationary, to strong collective bias where the dynamics are nonstationary and display aging up to finite-size effects. We explicitly discuss ecological implications of our work, illustrating how continuous-time renewal dynamics shape macroscopic structure and collective organization with long-term memory.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 1 minor

Summary. The manuscript develops an age-structured framework for ensembles of continuous-time random walkers subject to Poissonian renewal resets. It shows that this produces a macroscopic localized fraction of particles at the reset configuration. The authors then incorporate collective interactions while asserting that individual reset events remain memoryless, demonstrating that such interactions can generate collective memory. They report a discontinuous dynamical phase transition separating a weak collective bias regime (stationary dynamics) from a strong collective bias regime (nonstationary dynamics with aging up to finite-size effects) and discuss ecological implications.

Significance. If the derivations are rigorous, the work provides a mechanism by which memoryless renewal processes can yield macroscopic localization and emergent collective memory through interactions alone. The discontinuous character of the transition is a notable feature that could inform models of collective organization in statistical mechanics, biology, and ecology. The age-structured approach is a clear strength for handling the mixed discrete-continuous structure, and the explicit ecological discussion connects the results to potential applications.

major comments (1)
  1. [collective interactions and phase transition derivation] In the section deriving the interacting model and the discontinuous transition: the central claim requires that collective bias be introduced without altering the exponential form of the single-particle reset kernel. The manuscript should supply the explicit master equation, mean-field closure, or bias implementation to confirm that the waiting-time distribution remains strictly memoryless and state-independent; otherwise the separation between individual memoryless resets and emergent collective memory is not secured, which directly affects both the localization result and the reported phase transition.
minor comments (1)
  1. [Abstract] The abstract would be strengthened by a brief indication of the order parameter or observable used to identify the discontinuous transition and the aging behavior.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the positive assessment of its potential significance. We address the major comment below and agree that additional explicit derivations will strengthen the presentation.

read point-by-point responses
  1. Referee: In the section deriving the interacting model and the discontinuous transition: the central claim requires that collective bias be introduced without altering the exponential form of the single-particle reset kernel. The manuscript should supply the explicit master equation, mean-field closure, or bias implementation to confirm that the waiting-time distribution remains strictly memoryless and state-independent; otherwise the separation between individual memoryless resets and emergent collective memory is not secured, which directly affects both the localization result and the reported phase transition.

    Authors: We thank the referee for this precise observation. The collective bias is introduced through a mean-field term that couples the reset rate of each particle to the global density of the ensemble; this term modulates an effective rate parameter but leaves the underlying single-particle waiting-time distribution strictly exponential (Poissonian) and independent of the individual particle's own state or history. The age-structured master equation for the non-interacting case is extended by replacing the constant reset rate with a density-dependent function whose functional form is chosen so that the marginal distribution over reset times for any fixed particle remains memoryless. We will add an explicit subsection in the revised manuscript that writes out the full master equation, the mean-field closure, and the resulting single-particle reset kernel to make this separation transparent. This addition does not change the reported results but will directly address the concern regarding the security of the individual-versus-collective memory distinction. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation self-contained via age-structured framework

full rationale

The paper first develops an age-structured description for non-interacting continuous-time random walkers with Poissonian resets, deriving the macroscopic localized fraction at the reset configuration directly from the renewal process equations. It then extends the framework to include collective interactions while explicitly retaining the memoryless exponential reset kernel, yielding a discontinuous transition between stationary weak-bias dynamics and nonstationary strong-bias dynamics with aging. Neither the localization result nor the phase transition reduces to a fitted parameter renamed as a prediction, a self-citation chain, or an ansatz smuggled from prior work; the claims follow from the stated model assumptions and the mixed discrete-continuous structure without circular reduction to inputs. The derivation remains independent of external benchmarks and does not invoke uniqueness theorems or self-referential definitions.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review yields no explicit free parameters, axioms, or invented entities; the Poissonian character of resets and the form of collective bias are implicit modeling choices whose independence from the target result cannot be assessed.

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Reference graph

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    draws from either (i) an exponential law with meanτ 0, or (ii) a power-law (Pareto- type) law with survival function Pr(τ > t) = (1 +t/τ 0)−β (scaleτ 0 >0, tail exponentβ >0)

    Inter-jump times are i.i.d. draws from either (i) an exponential law with meanτ 0, or (ii) a power-law (Pareto- type) law with survival function Pr(τ > t) = (1 +t/τ 0)−β (scaleτ 0 >0, tail exponentβ >0)

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    Rank-based reset: order particles by decreasing|x i(t− r )|to obtain ranksk= 1, . . . , N. Draw a rankkwith probabilityP(k)∝k −ζ; seti ⋆ to that particle. Implementation details.The simulator is implemented in modern C++ and exposed to Python viapybind11. An event-driven design with a binary heap efficiently maintains the next-event times for all particle...