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arxiv: 2408.07049 · v3 · submitted 2024-08-13 · 🧮 math.PR

On the slow phase for fixed-energy Activated Random Walks

Pith reviewed 2026-05-23 22:19 UTC · model grok-4.3

classification 🧮 math.PR
keywords activated random walksslow phasetoppling procedureone-dimensional ringhigh density regimesleep rateinteracting particle systemsfixation time
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The pith

A toppling procedure on the ring builds an environment that sustains activity in high-density activated random walks for arbitrarily long times at any sleep rate.

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

The paper introduces a toppling procedure for the activated random walk model on the one-dimensional ring in the high-density regime. This procedure iteratively redistributes particles to construct configurations where the process remains active over extended periods. The construction works for arbitrarily large sleep rates and yields a direct proof that a slow phase exists. A sympathetic reader cares because the result clarifies the long-time behavior of the model without requiring external comparison arguments.

Core claim

On the one-dimensional ring in the high-density regime, a toppling procedure gradually builds an environment that can be used to show activity will be sustained for a long time. This establishes the existence of a slow phase for the activated random walk model for arbitrarily large sleep rates.

What carries the argument

The toppling procedure that gradually builds an environment sustaining activity for a long time.

If this is right

  • Activity persists for arbitrarily long times in the high-density regime.
  • The slow phase holds for every fixed sleep rate however large.
  • The argument applies directly to the fixed-energy version of the model on the ring.
  • The construction yields a self-contained proof without appeal to other techniques.

Where Pith is reading between the lines

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

  • The same toppling construction may adapt to periodic boundary conditions on higher-dimensional tori.
  • It could be used to produce explicit lower bounds on the time to absorption as a function of density.
  • The method might clarify whether the slow phase persists when the sleep rate grows with system size.

Load-bearing premise

The toppling procedure can be carried out indefinitely on the ring without the constructed environment eventually forcing all particles to sleep.

What would settle it

An explicit finite sequence of topplings on the ring that produces a configuration in which every particle eventually sleeps before time T for some fixed T independent of the number of steps taken.

Figures

Figures reproduced from arXiv: 2408.07049 by Bernardo N. B. de Lima, C\'elio Terra, Leonardo T. Rolla.

Figure 1
Figure 1. Figure 1: Example of possible state of a piece of the ring when an attempted emission is about [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
read the original abstract

We study the Activated Random Walk model on the one-dimensional ring, in the high density regime. We develop a toppling procedure that gradually builds an environment that can be used to show that activity will be sustained for a long time. This yields a self-contained and relatively short proof of existence of a slow phase for arbitrarily large sleep rates.

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

2 major / 2 minor

Summary. The manuscript claims to establish the existence of a slow phase for the fixed-energy Activated Random Walk model on the one-dimensional ring in the high-density regime, valid for arbitrarily large sleep rates. The argument proceeds via a toppling procedure that iteratively constructs an environment sustaining activity for arbitrarily long times; the proof is presented as self-contained.

Significance. If the central construction holds, the result supplies a relatively short, self-contained proof of the slow phase for large sleep rates. This would be a useful contribution to the literature on phase transitions for interacting particle systems, particularly as it avoids external parameters and focuses on the ring geometry.

major comments (2)
  1. [toppling procedure construction] The toppling procedure (described after the abstract and in the main construction) is asserted to produce sustained activity for arbitrarily long times. However, the argument that this procedure can be continued indefinitely on the finite ring—without eventually reaching a configuration in which all particles are asleep—is not made explicit. This step is load-bearing for the claim of an unbounded activity time, as termination at a fully sleeping state would cap the duration at a finite value.
  2. [main argument] The manuscript states that the procedure 'gradually builds an environment' that sustains activity, but does not provide a separate lemma or inductive step showing that each iteration preserves the possibility of further topplings without global sleep. On a closed ring this requires ruling out periodic or terminating traps; the current exposition leaves this as an implicit claim.
minor comments (2)
  1. [introduction] Notation for the sleep rate and density parameters could be introduced earlier and used consistently when stating the high-density regime.
  2. [toppling procedure] A brief diagram or schematic of one iteration of the toppling procedure would improve readability of the construction.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their detailed reading and for identifying points where the exposition of the toppling procedure requires greater explicitness. We agree that the argument for indefinite continuation on the finite ring needs to be made rigorous via additional lemmas, and we will revise the manuscript accordingly. Below we respond point by point to the major comments.

read point-by-point responses
  1. Referee: [toppling procedure construction] The toppling procedure (described after the abstract and in the main construction) is asserted to produce sustained activity for arbitrarily long times. However, the argument that this procedure can be continued indefinitely on the finite ring—without eventually reaching a configuration in which all particles are asleep—is not made explicit. This step is load-bearing for the claim of an unbounded activity time, as termination at a fully sleeping state would cap the duration at a finite value.

    Authors: We agree that the manuscript does not supply an explicit lemma or inductive argument establishing that the toppling procedure continues indefinitely without reaching a global sleeping configuration on the ring. This is a substantive gap in the current exposition. In the revised version we will insert a dedicated lemma (placed immediately after the description of the procedure) that proves, by induction on the number of iterations, that each toppling step produces a configuration containing at least one active particle whose subsequent motion on the ring cannot be trapped in a fully sleeping state before the next prescribed toppling. The lemma will explicitly rule out premature termination by tracking the net displacement of particles and the preservation of a positive density of active sites. revision: yes

  2. Referee: [main argument] The manuscript states that the procedure 'gradually builds an environment' that sustains activity, but does not provide a separate lemma or inductive step showing that each iteration preserves the possibility of further topplings without global sleep. On a closed ring this requires ruling out periodic or terminating traps; the current exposition leaves this as an implicit claim.

    Authors: We concur that the preservation of continued toppling possibility is left implicit and that the ring geometry introduces the possibility of periodic traps that must be excluded. The revision will add an inductive step (as a corollary to the new lemma mentioned above) showing that the environment constructed after k iterations always admits a configuration from which the (k+1)-st toppling can be performed without the system reaching a fully asleep state. The argument will use the one-dimensional structure to control the positions of sleeping particles and demonstrate that the toppling rule forces a net transport that prevents closure of all activity before the target time. revision: yes

Circularity Check

0 steps flagged

No circularity: self-contained mathematical construction with no reductions to inputs by definition or self-citation

full rationale

The paper develops an explicit toppling procedure to construct an environment on the 1D ring that sustains activity for arbitrarily long times, yielding a direct existence proof for the slow phase at high density and large sleep rates. No parameters are fitted to data, no predictions are made from subsets of the same data, and no load-bearing steps rely on self-citations or uniqueness theorems imported from the authors' prior work. The derivation is a standard constructive argument in probability that does not reduce any claimed result to its own inputs by construction; the indefinite extendability of the toppling is an internal verification step within the proof rather than a definitional loop. The result is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no free parameters, axioms, or invented entities are identifiable.

pith-pipeline@v0.9.0 · 5575 in / 903 out tokens · 20388 ms · 2026-05-23T22:19:01.028141+00:00 · methodology

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Reference graph

Works this paper leans on

15 extracted references · 15 canonical work pages

  1. [1]

    Asselah, N

    A. Asselah, N. Forien, and A. Gaudilli` ere. The critical density for activated random walks is always less than 1, 2022. arXiv:2210.04779

  2. [2]

    Asselah, L

    A. Asselah, L. T. Rolla, and B. Schapira. Diffusive bounds for the critical density of activated random walks. ALEA Lat. Am. J. Probab. Math. Stat. , 19:457–465, 2022

  3. [3]

    R. Basu, S. Ganguly, C. Hoffman, and J. Richey. Activated random walk on a cycle. Ann. Inst. Henri Poincar´ e Probab. Stat., 55:1258–1277, 2019

  4. [4]

    Bristiel and J

    A. Bristiel and J. Salez. Separation cutoff for activated random walks, 2022. arXiv:2209.03274

  5. [5]

    Cabezas and L

    M. Cabezas and L. T. Rolla. Avalanches in critical activated random walks. In In and out of equilibrium 3. Celebrating Vladas Sidoravicius , volume 77 of Progr. Probab., pages 187–205. Birkh¨ auser/Springer, Cham, 2021

  6. [6]

    N. Forien. Macroscopic flow out of a segment for activated random walks in dimension 1, 2024

  7. [7]

    Forien and A

    N. Forien and A. Gaudilli` ere. Active phase for activated random walks on the lattice in all dimensions, 2022. arXiv:2203.02476

  8. [8]

    Hoffman, Y

    C. Hoffman, Y. Hu, J. Richey, and D. Rizzolo. Active phase for the stochastic sandpile on z,

  9. [9]

    Hoffman, T

    C. Hoffman, T. Johnson, and M. Junge. The density conjecture for activated random walk,

  10. [10]

    Hoffman, J

    C. Hoffman, J. Richey, and L. T. Rolla. Active phase for activated random walk on Z. Comm. Math. Phys., 399:717–735, 2023

  11. [11]

    Y. Hu. Active phase for activated random walk on Z2, 2022. arxiv:2203.14406

  12. [12]

    Levine and V

    L. Levine and V. Silvestri. How far do activated random walkers spread from a single source? J. Stat. Phys. , 185:18, 2021

  13. [13]

    Podder and L

    M. Podder and L. T. Rolla. Uniform threshold for fixation of the stochastic sandpile model on the line. J. Stat. Phys. , 182:52, 2021

  14. [14]

    L. T. Rolla. Activated random walks on Zd. Probab. Surv., 17:478–544, 2020

  15. [15]

    L. Taggi. Essential enhancements in Abelian networks: Continuity and uniform strict mono- tonicity. Ann. Probab., 51:2243–2264, 2023. 12