REVIEW 2 major objections 5 minor 1 cited by
Asymptotic behavior of the generalized Derrida-Retaux recursive model
T0 review · 2 major / 5 minor · reviewed 2026-08-12 · deepseek-v4-flash
Pith's one-line read The paper derives sharp asymptotic expansions for the parameters of the generalized Derrida–Retaux model with geometric offspring, including a critical regime with a log n/n^2 correction, and obtains the sustainability probability to…
desk verdict Solid, self-contained contribution to the Derrida–Retaux program, but the advertised critical log correction has a sign error that makes Theorem 1.3(3) and the critical corollaries false as stated. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central object is the two-parameter family of geometric-type laws $G(r,p)$, with atom $p$ at the origin and a geometric tail with ratio $1-r$ on the positive integers. The load-bearing identity is the recurrence (1.7) and its consequence (2.8), $$\frac1{r_{n+2}}-\frac1{r_{n+1}}=m(1-r_{n+1})\left(\frac1{r_{n+1}}-\frac1{r_n}\right),$$ which lets the authors convert local difference estimates into global asymptotic expansions by the Stolz–Cesàro theorem. In the critical case the proof works with the displacement $v_n=r_n-(1-m^{-1})$ and the identity (3.18), which isolates the excess of $1/v_{n+1}-1/v_n$ over $m/2$; this is what produces the logarithmic correction.
What would settle it
Iterate the recurrence (1.7) numerically for $m=2$ from any initial pair whose limits are $r_*=1/2$ and $p_*=1$, and compute $n^3(v_n-v_{n+1}-v_n v_{n+1})$ with $v_n=r_n-1/2$; Theorem 1.3 requires this to converge to $2$, so any other long-run value would refute the expansion.
Extended reading notes
Core claim
The central claim is Theorem 1.3: for geometric offspring, the two-parameter geometric-type family $G(r,p)$ is preserved under the recursion, and the parameters converge to one of three regimes. In the critical regime $r_*=1-m^{-1}$, $p_*=1$, the parameters obey $$r_n = 1-\frac1m+\frac{2}{mn}-\frac{4(m+1)\log n}{3m(m-1)$n^{2}$}+o\!\left(\frac{\log n}{$n^{2}$}\right),\qquad p_n = 1-\frac{2}{(m-1)^$2n^{2}$}-\frac{8(m+1)\log n}{3(m-1)^$3n^{3}$}+o\!\left(\frac{\log n}{$n^{3}$}\right).$$ From these expansions the paper derives the sharp sustainability probability, the conditional geometric limit law, the first moment, and the probability generating function. The critical conditional law matches the earlier deterministic-offspring conjecture, but the decay prefactors differ because of randomness in the number of offspring.
Load-bearing premise
Everything rests on the offspring law being exactly geometric, $\mathbb{P}(\eta=n)=(1/m)(1-1/m)^{n-1}$; this is what keeps every marginal inside the two-parameter geometric-type family, and without it the recurrence (1.7) and all expansions that follow would not hold.
Editorial extensions
If this is right
- In the critical regime the sustainability probability obeys $\mathbb{P}(Y_n\ge1)=2/((m-1)^2n^2)+8(m+1)\log n/(3(m-1)^3n^3)+o(\log n/n^3)$.
- The conditional law $\mathbb{P}(Y_n=k\mid Y_n\ge1)$ converges to $(1-1/m)(1/m)^{k-1}$ in the critical case, matching the deterministic-offspring conjecture (C2).
- The first moment in the critical case is $\mathbb{E}(Y_n)=2m/((m-1)^3n^2)+8m(m+1)\log n/(3(m-1)^4n^3)+o(\log n/n^3)$.
- The critical generating function at $s=m$ behaves like $\mathbb{E}(m^{Y_n})=1+1/((m-1)n)+2(m+1)\log n/((m-1)^2n^2)+o(\log n/n^2)$.
- The prefactors differ systematically from the fixed-offspring conjectures (C1), (C3), (C4a), (C4b), and the paper attributes the slowdown to randomness in the offspring number.
Reading between the lines
- The same two-parameter closure and Stolz–Cesàro summation should transfer to the exponential-type marginals mentioned in Remark 1.12, yielding analogous critical $(\log n)/n^2$ corrections in the continuous-time analogue.
- The geometric-law prefactors likely encode the variance of the offspring distribution; comparing the coefficients with the deterministic $m$ case suggests a testable dependence on the second moment of $\eta$.
- The remainder constant in (3.19), namely $4(m+1)/(3m(m-1))$, is a sharp numerical diagnostic: for $m=2$ it equals $2$, so direct iteration of the recurrence provides an unambiguous check of the whole asymptotic program.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies the generalized Derrida–Retaux process (1.3) under a geometric offspring distribution (1.6). It proves that the class of geometric-type marginal distributions is preserved, reducing the model to the two-parameter recursion (1.7), and it characterizes the three regimes through the limits (r*, p*). The main results are asymptotic expansions of r_n and p_n in the supercritical, subcritical, and critical cases (Theorem 1.3), with consequences for the sustainability probability, first moment, and probability generating function (Corollaries 1.5, 1.8, 1.9) and for the conditional limit laws (Corollary 1.6). The critical-case analysis contains nontrivial logarithmic corrections, and the proofs are based on generating-function recursions, the preservation theorem, and Stolz–Cesàro limit arguments.
Significance. If the stated results were correct, the paper would give the sharp critical scaling for the geometric-offspring version of the model, including the constants in front of the log n/n^2 and log n/n^3 corrections, and would refine the conjectures (C1)–(C4b) for this solvable family. The proof strategy is largely self-contained, does not use fitted parameters, and the preservation theorem for geometric-type distributions is elegant. However, the advertised asymptotic constants contain sign and algebraic errors in two central places, so the paper cannot be accepted without correction.
major comments (2)
- [Theorem 1.3(3), Corollaries 1.5(3), 1.8(3), 1.9(3)] Section 3, Theorem 1.3(3): the sign of the log n/n^3 term in the critical p_n expansion is wrong. From (3.21), v_n = r_n - (1 - 1/m) = 2/(mn) - A log n/n^2 with A = 4(m+1)/(3m(m-1)); hence v_n - v_{n+1} = 2/(m n^2) - 2A log n/n^3 + o(log n/n^3), as in (3.23). Identity (2.9) then gives 1 - p_n = (v_n - v_{n+1})/((m-1)(1 - 1/m + v_{n+1})) = 2/((m-1)^2 n^2) - 8(m+1)/(3(m-1)^3) log n/n^3 + o(log n/n^3), so p_n = 1 - 2/((m-1)^2 n^2) + 8(m+1)/(3(m-1)^3) log n/n^3 + o(log n/n^3). The theorem states the opposite sign, while the proof's own displayed line after (3.24) has the correct minus sign in 1 - p_n. Consequently Corollary 1.5(3) should have the negative log term, Corollary 1.8(3) should have the negative log coefficient, and both displays in Corollary 1.9(3) need corrected signs; in particular (1.15) should read E(m^{Y_n}) = 1 + 1/((m-1)n) - 2(m+1)/(3(m-1)^2) log n/n^2 + o(log n/n^2).
- [Theorem 1.3(2), Corollaries 1.5(2), 1.8(2), 1.9(2)] Section 3, Theorem 1.3(2): the second-order subcritical coefficients are algebraically wrong. Using (3.8), d_n = r_n - r_{n+1} = K_n gamma_*^n r_n r_{n+1}, with K_n = K + mK^2 r_*^2/(1 - gamma_*)^2 gamma_*^n + o(gamma_*^n) and r_n = r_* + K r_*^2/(1 - gamma_*) gamma_*^n + o(gamma_*^n), gives d_n = K r_*^2 gamma_*^n + K^2 r_*^3 (1 - gamma_*^2 + m r_*)/(1 - gamma_*)^2 gamma_*^{2n} + o(gamma_*^{2n}). Summing yields r_n = r_* + K r_*^2 gamma_*^n/(1 - gamma_*) + K^2 r_*^3 (1 - gamma_*^2 + m r_*)/[(1 - gamma_*)^2 (1 - gamma_*^2)] gamma_*^{2n} + o(gamma_*^{2n}), not the displayed (1 + m r_*)/[(1 - gamma_*^2)(1 - gamma_*)^2]. Equivalently, from (2.9), 1 - p_n = K r_* gamma_*^n/(m - 1) + K^2 r_*^2 (1 - gamma_* + m r_*)/[(m - 1)(1 - gamma_*)^2] gamma_*^{2n} + o(gamma_*^{2n}), so p_n should have minus this second term. The same correction propagates to Corollaries 1.5(2), 1.8(2), and 1.9(2); for example, the gamma_*^{2n} coefficient in Corollary 1.8(2) should be mK^2 r_*^2/[(m - 1)(1 - gamma_*)^2], not mK^2 r_*/[(m - 1)(1 - gamma_*)^2].
minor comments (5)
- [Lemma 3.2] The opening sentence contains a typo: 'The the approach' should read 'The approach'.
- [Proof of Theorem 1.3(3)] The displayed identity after (3.23) writes m/2 v_n v_{n+1} = m/2 v_n^2 + m/2 v_n(v_n - v_{n+1}); the sign before the second term should be minus. This does not affect the order shown, but the line should be corrected.
- [Lemma 3.1] The statement 'v_n strictly decreases to zero' should be qualified: in the critical case r_n decreases to r_*, so v_n = r_n - r_* decreases to zero from above; if the initial value put v_n below zero, the wording needs an index shift.
- [Remark 1.11] The comparison of the critical constants with the conjectures (C1), (C3), (C4a), and (C4b) should be revisited after the sign corrections, since the sign of the logarithmic correction changes the qualitative comparison.
- [References and formatting] Reference [15] and the proof of Corollary 1.8 contain missing spaces ('Derrida–Retauxtypemodels', 'Inthesubcriticalcase'), and the proof of Corollary 1.6(1) would benefit from a brief justification of the interchange of limits.
Circularity Check
No significant circularity: the asymptotic expansions are solved from the exact recursion, not assumed or fitted.
full rationale
The paper's derivation chain is self-contained. Theorem 1.1 proves, rather than assumes, the closure of geometric-type laws under the recursion, using the generating function identity (2.1) and the geometric offspring law (1.6). Proposition 2.2 derives the key exact difference equation (2.8), and Theorem 1.3 solves this equation via the Stolz–Cesàro theorem and Taylor expansions. The constants F∞ and K are defined by convergent infinite products over the already-converging sequences (1.9) and (1.10), so no fitted or externally imposed parameter is renamed as a prediction. The corollaries are exact rearrangements: P(Yn ≥ 1) = 1 − pn, E(Yn) = (1 − pn)/rn, and the generating function formula (2.1), so they are consequences of Theorem 1.3 rather than inputs to it. The only self-citation, [15] in the introduction, is contextual and not load-bearing for any theorem. No uniqueness theorem from the authors' prior work is invoked to force a choice, and no ansatz is imported by citation. A skeptical reviewer has noted a possible sign error in the log n/n^3 coefficient of pn in Theorem 1.3(3); if real, that is an arithmetic/correctness flaw, but it is not circularity because the displayed expansion is still derived from (2.9), (3.21), and (3.23), not assumed. The analysis therefore earns a score of 0.
Assumptions & free parameters
assumptions (5)
- standard math Stolz-Cesàro theorem is applicable to the difference sequences derived from (1.7).
- standard math Taylor expansions of exp, log, and 1/(1±x) hold for the small remainder terms.
- standard math Borel-Cantelli lemma for almost sure convergence of Y_n.
- domain assumption The offspring number η has a geometric distribution with mean m: P(η=n) = (1/m)(1-1/m)^{n-1}, n ≥ 1.
- domain assumption The initial distribution is µ0 = G(r0,p0) with (r0,p0) ∈ (0,1)^2, and {Y_{n,k}} are independent copies of Y_n independent of η.
Cite this review
Pith. "Pith review of Asymptotic behavior of the generalized Derrida-Retaux recursive model." pith.science (2026). https://pith.science/paper/5HUERBM5
@misc{pith2026241113068,
author = {Pith},
title = {Pith review of: Asymptotic behavior of the generalized Derrida-Retaux recursive model},
year = {2026},
howpublished = {\url{https://pith.science/paper/5HUERBM5}},
note = {Machine review of arXiv:2411.13068}
}
read the original abstract
We study the max-type recursive model introduced by Hu and Shi (J. Stat. Phys., 2018), which generalizes the model of Derrida and Retaux (J. Stat. Phys., 2014). The class of geometric-type marginal distributions is preserved by the model with a geometric offspring distribution. We give some long-time asymptotic expansions of the parameters of the marginal distribution. From the expansions, we derive the asymptotics of the sustainability probability, marginal distribution, first moment and probability generating function.
Forward citations
Cited by 1 Pith paper
-
Derrida-Retaux type models and related scaling limit theorems
Rescaled generalized Derrida-Retaux dynamics converge in Skorokhod space to a continuous-time process whose semigroup, generator, and martingale problem are characterized.
Reference graph
Works this paper leans on
-
[1]
and Bandyopadhyay, A.: A survey of max-type recursive distributional equations
Aldous, D.J. and Bandyopadhyay, A.: A survey of max-type recursive distributional equations. Ann. Appl. Probab. 15, 1047–1110 (2005)
work page 2005
-
[2]
The Derrida-Retaux model on a geometric Galton-Watson tree
Alsmeyer, G.; Hu, Y. and Mallein, B.: The Derrida–Retaux model on a geometric Galton- Watson tree.Preprint (2025+). Available at arXiv:2502.02991
work page Pith review arXiv 2025
-
[3]
Chen, X.: Infinite differentiability of the free energy for a Derrida–Retaux system.Preprint (2024+). Available at arXiv:2405.09741. 18
arXiv 2024
-
[4]
and Shi, Z.: Derrida–Retaux conjecture on recursive models.Ann
Chen, X.; Dagard, V.; Derrida, B.; Hu, Y.; Lifshits, M. and Shi, Z.: Derrida–Retaux conjecture on recursive models.Ann. Probab. 49 (2021), 637–670
work page 2021
-
[5]
and Shi, Z.:A max-type recursive model: Some properties and open questions
Chen, X.; Derrida, B.; Hu, Y.; Lifshits, M. and Shi, Z.:A max-type recursive model: Some properties and open questions . In: Sojourns in Probability Theory and Statistical Physics-III (2019), 166–186. Springer, Singapore
work page 2019
-
[6]
and Shi, Z.: The sustainability probability for the critical Derrida–Retaux model
Chen, X.; Hu, Y. and Shi, Z.: The sustainability probability for the critical Derrida–Retaux model. Probab. Theory Related Fields 182 (2022), 641–684
work page 2022
-
[7]
and Martin, A.: A spin glass with random couplings.J
Collet, P.; Eckmann, J.P.; Glaser, V. and Martin, A.: A spin glass with random couplings.J. Stat. Phys 36 (1984), 89–106
work page 1984
-
[8]
and Martin, A.: Study of the iterations of a mapping associated to a spin-glass model.Commun
Collet, P.; Eckmann, J.P.; Glaser, V. and Martin, A.: Study of the iterations of a mapping associated to a spin-glass model.Commun. Math. Phys. 94 (1984), 353–370
work page 1984
Show all 15 references
-
[9]
and Hénard, O.: The phase transition for parking on Galton–Watson trees.Discrete Anal
Curien, N. and Hénard, O.: The phase transition for parking on Galton–Watson trees.Discrete Anal. (2022), Paper No. 1, 17 pp
2022
-
[10]
Derrida, B and Retaux, M.: The depinning transition in presence of disorder: a toy model.J. Stat. Phys. 156 (2014), 268–290
2014
-
[11]
and Przykucki, M.: Parking on a random tree.Comb
Goldschmidt, C. and Przykucki, M.: Parking on a random tree.Comb. Probab. Comput. 28 (2019), 23–45
2019
-
[12]
and Pain, M.: An exactly solvable continuous-time Derrida–Retaux model, Commun
Hu, Y.; Mallein, B. and Pain, M.: An exactly solvable continuous-time Derrida–Retaux model, Commun. Math. Phys. 375 (2020), 605–651
2020
-
[13]
and Shi, Z.: The free energy in the Derrida–Retaux recursive model.J
Hu, Y. and Shi, Z.: The free energy in the Derrida–Retaux recursive model.J. Stat. Phys. 172 (2018), 718–741
2018
-
[14]
and Rogers, T.D.: Asymptotic behavior for iterated functions of random variables
Li, D. and Rogers, T.D.: Asymptotic behavior for iterated functions of random variables. Ann. Appl. Probab. 9 (1999), 1175–1201
1999
-
[15]
Preprint (2024+)
Li, Z.andZhang, R.: Derrida–Retauxtypemodelsandrelatedscalinglimittheorems. Preprint (2024+). Available at arXiv:2411.12189. 19
2024 arXiv
Reviewed August 12, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.