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Limit law for root separation in random polynomials

T0 review · 3 major / 3 minor · reviewed 2026-08-16 · deepseek-v4-flash

Pith's one-line read At scale $n^{-5/4}$, the pairwise gaps among roots of a random polynomial converge to a Poisson process with an explicit cubic intensity.

desk verdict A substantial paper that likely resolves the n^{-5/4} root-separation problem for sub-Gaussian Kac polynomials, but the printed event A_z(U) has a sign error that makes the proof as written inconsistent until fixed. read the letter →

arxiv 2505.02723 v1 pith:UJSBUBRR submitted 2025-05-05 math.PR math.CAmath.CV

classification math.PRmath.CAmath.CV MSC 60G5560F0530C1530B20
keywords randompolynomialsKacrootseparationPoissonpointprocesssmallballprobabilityuniversalitydoublerootsLittlewood
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

This paper establishes a precise limit law for how close the roots of a random polynomial can come to one another. For a Kac polynomial $f_n(z)=\sum_{k=0}^n \xi_k z^k$ whose coefficients are independent, identically distributed, mean-zero, and sub-Gaussian with no atom at zero, the paper proves that the collection of pairwise root distances, magnified by $n^{5/4}$, converges in distribution to a non-homogeneous Poisson process on the nonnegative reals with intensity $c_* t^3\,dt$ for an explicit positive constant $c_*$. The exponent $5/4$ is the paper's central quantitative finding: it encodes the repulsion between roots, which pushes the natural close-pair scale from $n^{-3/2}$ (what independent points in the same annulus would produce) up to $n^{-5/4}$. A corollary gives the first limit law for the minimal distance between distinct roots, and the proof includes a standalone theorem stating that a random Taylor series with i.i.d. coefficients almost surely has no double zero away from the origin.

What carries the argument

The argument is carried by a net reduction in the bulk annulus $\Omega_K=\mathbb{H}\cap A(1-K/n,1+K/n)$, where almost all roots lie. At scale $\delta=n^{-5/4-\beta}$, each net point $z$ is interrogated through the random triple $(f_n(z),f_n'(z),f_n''(z))$: the linear root prediction $z - f_n(z)/f_n'(z)$ must land in the polar cell $R_z^\circ$, and the quadratic second-root prediction $2|f_n'(z)|/|f_n''(z)|$ must land in $n^{-5/4}U$. A close pair of roots forces both events, and conversely the quadratic approximation recovers the pair from them, giving the two-sided counting identity that reduces the Poisson limit to a method-of-moments computation over the net. To control small-ball probabilities for arbitrary coefficient laws, net points are split into 'smooth' points (angles $\theta$ with no $p\theta/\pi$ close to an integer for small $p$, so that the coefficient vector is genuinely high-dimensional) where a Konyagin-Schlag / Cook-Nguyen style local Gaussian comparison (Theorem 3.12) shows asymptotic agreement with Gaussian coefficients, and 'rough' points handled by cruder arithmetic small-ball bounds. The limiting intensity emerges from an explicit Gaussian computation of the event $A_z(U)$: the function $F(x)$ of (78) integrates to give $c_*(K)=\tfrac14\int_{-K}^K F(x)\,dx$ and $c_*=\lim_{K\to\infty}c_*(K)$. Pairs of roots well inside the unit disk are killed by the almost-sure no-double-zero theorem for random Taylor series, so the entire limiting process is driven by the $1/n$-neighborhood of the unit circle.

What would settle it

Run the theorem's own simulation: for Rademacher or standard-Gaussian coefficients at degree $n=10^4$, sample the unnormalized pair-distance process and check that the expected number of pairs with $n^{5/4}|\alpha_j-\alpha_j'|\le s$ grows like $c_*s^4/4$ and that $P[n^{5/4}m_n\ge s]$ converges to $\exp(-c_*s^4/4)$; any statistically clear deviation from the quartic power law refutes the $t^3$ intensity and the minimal-gap corollary. A second test: replace real coefficients with i.i.d. complex Gaussians and see whether the same Poisson limit survives, which would settle whether the real-coefficient conjugation step in Section 3 is essential.

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Extended reading notes

Core claim

The central claim (Theorem 1.1) is that for $f_n(z)=\sum_{k=0}^n \xi_k z^k$ with i.i.d. mean-zero sub-Gaussian coefficients and $P[\xi_0=0]=0$, the point process $\{n^{5/4}|\alpha_j-\alpha_j'| : 1\le j<j'\le n\}$ converges vaguely to a non-homogeneous Poisson point process on $\mathbb{R}_{\ge 0}$ with intensity $c_* t^3\,dt$. The cubic shape of the intensity is universal: it depends on the coefficient law only through the positive constant $c_* = \tfrac{1}{4}\int_{-\infty}^{\infty}F(x)\,dx$, where $F$ is given by an explicit Gaussian computation. An immediate corollary is that the minimal separation $m_n$ between roots obeys $\lim_{n\to\infty} P[n^{5/4}m_n\ge s] = \exp(-c_*s^4/4)$, so double roots become asymptotically improbable for every coefficient law covered by the theorem. En route, Theorem 1.3 proves that a random Taylor series with i.i.d. coefficients satisfying $E\log(1+|a_0|)<\infty$ satisfies $P[\exists\alpha\in\mathbb{D}: F(\alpha)=F'(\alpha)=0] = (P[a_0=0])^2$, i.e. a double zero can occur only at the origin and only when the first two coefficients vanish.

Load-bearing premise

The coefficients must be real-valued for the proof as written: the upper-half-plane reduction and the identification of the limiting distance set both use the conjugation identity $f_n(z)=\overline{f_n(\bar z)}$, yet Theorem 1.1 as stated never says that the coefficients are real.

Editorial extensions

If this is right

  • The minimal separation $m_n$ between roots satisfies $P[n^{5/4}m_n\ge s]\to\exp(-c_*s^4/4)$: a nontrivial, universal limit law for how close the two closest roots can be.
  • Double roots become asymptotically improbable for every mean-zero sub-Gaussian coefficient law with no atom at zero, which the paper notes is the first such statement for Kac polynomials beyond Gaussian or integer-valued coefficient distributions.
  • The entire pairwise-distance spectrum is universal: only the constant $c_*$ depends on the coefficient law, while the $t^3$ intensity shape is fixed by the geometry of the bulk annulus.
  • Roots that remain a fixed distance inside the unit disk are uniformly separated with high probability, so the limiting statistics are governed entirely by roots within distance $K/n$ of the unit circle.
  • As a byproduct, Theorem 1.3 states that a random Taylor series with i.i.d. coefficients has no double zero away from the origin almost surely, extending a previously known Gaussian special case to all coefficient laws with finite $E\log(1+|a_0|)$.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • A direct extension the paper leaves implicit: for i.i.d. complex coefficients the same $t^3$ Poisson law should hold with a possibly different constant, since the upper-half-plane reduction would be unnecessary; a complex-Gaussian simulation would show whether the conjugation symmetry in Section 3 is essential or merely organizational.
  • The $(n\varepsilon)^2$ repulsion factor is a transferable template: any planar point field whose pair correlation carries such a factor at scales $\varepsilon\gg n^{-1}$ should exhibit the same $n^{-5/4}$ close-pair scale and $t^3$ distance intensity, and this paper supplies the first rigorous instance for random roots.
  • The constant $c_*=\tfrac14\int_{-\infty}^{\infty}F(x)\,dx$, explicit in principle through (78), is never evaluated numerically; computing it to a few digits would turn Theorem 1.1 into a quantitative prediction that numerical experiments on the minimal gap could confirm to several digits.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 3 minor

Summary. The paper studies Kac polynomials with i.i.d. mean-zero sub-Gaussian coefficients and proves that the set of n^{5/4}-scaled pairwise root distances converges vaguely to a non-homogeneous Poisson point process on R_{\ge 0} with intensity c_* t^3 dt, for an explicit positive constant c_*. The proof reduces the problem to net counts in the annulus near the unit circle, uses small-ball probability estimates for (f_n, f'_n, f''_n) at 'smooth' points, compares these statistics with Gaussian ones for separated tuples, and computes the intensity by a Gaussian calculation. A separate result (Theorem 1.3) states that a random Taylor series with log-integrability has no double zeros inside the unit disk almost surely, except possibly at the origin with probability P[a_0=0]^2.

Significance. If the identified issues are corrected, this is a substantial universality result: root separation is one of the few genuinely pairwise quantities of random polynomials for which a full distributional limit is obtained beyond Gaussian models, and the explicit form c_* t^3 yields a limit law for the minimal separation (Corollary 1.2). The proof is a coherent chain of reductions, and Theorem 1.3 is self-contained and of independent interest. The intensity c_* is defined by an explicit positive integral rather than fitted, and the small-ball/Gaussian-comparison machinery is developed in detail. The current version, however, contains a sign inconsistency in the central event and a mismatch in the definition of the counting statistic; these are correctable but load-bearing.

major comments (3)
  1. [Section 5, Eqs. (50), (55), (56); see also (67) and (133)] The events A_z(U), A^+_z(U), and A^-_z(U) are defined with f_n(z)/f'_n(z) - z in R^\circ_z or the analogous rectangles, but every root-locating statement in Section 5 requires the opposite sign: Claim 5.5 concludes z - f_n(z)/f'_n(z) in R^\sharp_z, while Claim 5.6 and Lemma 5.7 use z - f_n(z)/f'_n(z) in R_z. On the good event G from (53) together with |f'_n(z)| \ge n^{5/4}/\log n, the printed event forces |f_n(z)| = |f_n(z)/f'_n(z)| |f'_n(z)| \asymp 2|z| n^{5/4}/\log n, contradicting the bound |f_n(z)| \le n^{1/2} \log^2 n. Moreover, the Gaussian computation in Section 10, especially (136), conditions on F_n(w)/F'_n(w) lying in a small rectangle around 0, which is the event z - f_n(z)/f'_n(z) \in R^\circ_z and not the displayed event. Thus, as written, Proposition 5.3 and the moment computation in Section 6 establish Poisson limits for two different counting events; the reduction to the net is valid only after the sign in (50), (55), (56), (67), and (133) is corrected.
  2. [Section 3, Eq. (23); proof of Theorem 1.1] The definition of X_n(U) in (23) counts the number of roots \alpha \in \Omega_K that have some root \alpha' at distance in n^{-5/4}U, so each close pair contributes two to X_n(U). The proof of Proposition 5.3 and the proof of Theorem 1.1 treat X_n(U) as the number of unordered pairs of roots at such a distance: X^\pm_n(U) in (57) sum over unordered pairs, and the proof of Theorem 1.1 identifies \mu^K_n(U) with X_n(U). These two quantities differ by a factor of two. Since the intensity c_*(K) is defined and computed for the pair count (see Claim 6.6 and the factor 2^{-m} in (84)), the statement of Theorem 3.2 is inconsistent with definition (23). The definition should be corrected to count unordered pairs, or all prefactors and the limiting intensity must be rescaled consistently.
  3. [Theorem 1.1 and Section 3] Theorem 1.1 does not state that the coefficients are real-valued, but the proof relies on this: Section 3 begins with the symmetry statement for real coefficients and defines X_n(U) using only roots in the upper half-plane H, and the proof of Theorem 1.1 uses only roots in H. Without the real-coefficient assumption, the symmetry argument and the identification of the limiting process with distances between H-roots fail. Either add the real-coefficient hypothesis to Theorem 1.1, the abstract, and Corollary 1.2, or provide an argument that covers complex coefficients.
minor comments (3)
  1. [Proof of Lemma 4.3] The subscripts in the four sums in the proof are inconsistent with the definitions in (34) and (35): the sums labelled N^{(1)}_s, N^{(2)}_s, and N^{(3)}_s should be over the non-smooth parts N^{(1)}_{ns}, N^{(2)}_{ns}, and N^{(3)}_{ns}.
  2. [Section 3] The sentence 'Since f_n has real coefficients, f_n(z) = f_n(z)' should read f_n(z) = \overline{f_n(\bar z)}; as printed it is either a typographical error or an empty identity.
  3. [Abstract] The abstract states only that the coefficients are independent and identically distributed, omitting the mean-zero, sub-Gaussian, and real-coefficient hypotheses used in Theorem 1.1; the abstract should state the assumptions that are actually proved.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the Poisson intensity is computed from an explicit Gaussian integral, not fitted, and the proof is self-contained against external benchmarks.

full rationale

The derivation of Theorem 1.1 is not circular. The limit object is reduced to Theorem 3.2, where the intensity lambda_{K,U} = c_*(K) integral_U t^3 dt is computed from first principles: c_*(K) is defined by (68) as an explicit integral of the function F(x) from (78), and Section 10 evaluates the Gaussian small-ball probability (133)-(137) directly; no parameter is fitted to the separation data, and the t^3 factor arises from the change of variables in the Gaussian computation rather than being imported from the conclusion. The net reduction in Sections 5-6 is justified by Rouché-type claims (Claims 5.5-5.7, Lemma 5.8), and the moment bounds use Gaussian comparison and small-ball estimates proved in Sections 7-9. Cited results by the same authors are used as technical tools, not as premises containing the separation theorem: in particular, [Coo+23, Lemma 3.5] is invoked only as a routine Gaussian comparison for densities after the covariance block structure is derived in (128), and [MS20] and [Cam+24] serve as background or technical input. Theorem 1.3 is proved independently in Section 2. The apparent sign mismatch between the displayed event (50) and the z - fn/f' condition used in Claims 5.5-5.6, as well as the unspecified real-coefficient assumption, are correctness risks rather than circularity: they do not make the derived quantity equal to an input by definition.

Assumptions & free parameters 2 free parameters · 5 assumptions · 0 invented entities

No new physical entities or fitted constants are introduced. The limiting intensity c_* is defined by an explicit integral of a positive smooth function F(x), which is computed in Section 10 from Gaussian small-ball probabilities. The proof introduces technical constants tau and beta, but these are universal small constants chosen for convenience and do not alter the result.

free parameters (2)
  • tau = 10^{-4}
    A sufficiently small absolute constant used in the net arguments and in the definition of smoothness (A = d^{7 tau}). It is chosen by hand (the paper says 'taking tau = 10^{-4} ... is fine') and does not affect the final constant.
  • beta = tau/20 = 5*10^{-6}
    A small absolute constant controlling the net mesh delta = n^{-5/4-beta} and the thin boundary layers. Chosen for convenience in the proof; it is universal and does not enter the limit intensity.
assumptions (5)
  • domain assumption The coefficients xi_0,...,xi_n are i.i.d., mean-zero, sub-Gaussian, and P[xi_0 = 0] = 0.
    This is the standing assumption of Theorem 1.1 and is used throughout for small-ball bounds and for the Gaussian comparison.
  • domain assumption The coefficients are real-valued, so f_n(z) = f_n(bar z) and roots are conjugate-symmetric.
    Invoked in Section 3 to restrict to the upper half-plane H and to define X_n(U). This assumption is not stated in Theorem 1.1.
  • standard math Classical tools: Esseen inequality, Levy-Kolmogorov-Rogozin anti-concentration, Rouche's theorem, Hurwitz's theorem, Jensen's bound, Salem-Zygmund inequality.
    These are standard imported results used in Sections 2, 3, 4 and 9. They are cited to [Ess66], [Ess68], [Kah85], and standard references.
  • domain assumption The effective degree d_n(z) = min{n, (1-|z|)^{-1}} controls the local behavior of f_n at z.
    Used in the small-ball bounds in Sections 7 and 8. In the annulus Omega_K, d_n(z) is comparable to n, which is asserted in Remark 3.11.
  • standard math The Riemann sum approximation of the integral of F in Claim 6.6 converges uniformly for K in compact sets.
    The proof uses a Riemann sum over a net whose spacing tends to 0; this relies on the differentiability and decay properties of F established in Claim 6.5.

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Pith. "Pith review of Limit law for root separation in random polynomials." pith.science (2026). https://pith.science/paper/UJSBUBRR

@misc{pith2026250502723,
  author       = {Pith},
  title        = {Pith review of: Limit law for root separation in random polynomials},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/UJSBUBRR}},
  note         = {Machine review of arXiv:2505.02723}
}
abstract

Let $f_n$ be a random polynomial of degree $n\ge 2$ whose coefficients are independent and identically distributed random variables. We study the separation distances between roots of $f_n$ and prove that the set of these distances, normalized by $n^{-5/4}$, converges in distribution as $n\to \infty$ to a non-homogeneous Poisson point process. As a corollary, we deduce that the minimal separation distance between roots of $f_n$, normalized by $n^{-5/4}$ has a non-trivial limit law. In the course of the proof, we establish a related result which may be of independent interest: a Taylor series with random i.i.d. coefficients almost-surely does not have a double zero anywhere other than the origin.

Figures

Figures reproduced from arXiv: 2505.02723 by the authors.

Figure 1
Figure 1. Left: roots on the unit circle of Re(fn) for random Littlewood fn (red points); Right: the same number of i.i.d. uniform points on the unit circle (blue points). via the Kac-Rice formula for the 2-point function of the random roots, see for example [Hou+09, Chapter 3.4] or [SZ03, Theorem 4]. One of the main achievements of this paper is obtaining the asymptotic (4) for a large class of coefficients distribution for … view at source ↗

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Law of large numbers for the discriminant of random polynomials

    math.PR 2025-06 conditional novelty 8.0 of 10

    Random Kac polynomials have discriminant |Δ(f_n)| = n^{2n} e^{-D_* n(1+o(1))} with an explicit universal constant D_* ≈ 5.92947.

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