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White 2022 erdos minimum overlap problem

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Ethan Patrick White, Erdős' minimum overlap problem. arXiv:2201.05704 (2022).

For a partition of [2n] into equal halves A and B, Erdős asked for the size of M(n) = min max_k |{(a,b) in A x B : a - b = k}|; Haugland showed M(n)/n tends to a constant mu, and before this work sqrt(4 - sqrt 15) = 0.356394 <= mu <= 0.380927 (Moser's lower bound, Haugland's upper bound). White's Theorem 1 proves mu >= 0.379005, so the remaining gap is about 0.5 percent. White works with the continuous analog of Moser and Murdeshwar, shown by Swinnerton-Dyer to have the same value mu: minimize the sup norm of M(x) = int f(t) g(x+t) dt over measurable f: [-1,1] -> [0,1] with g = 1 - f and integral of f equal to 1. The method is elementary Fourier analysis, deriving linear constraints on the Fourier coefficients of M (starting from the fact that M integrates to 1, hence mu >= 0.25) and turning the resulting relaxation into a convex optimization program solved numerically; more computation would improve the bound further. For problem 36, Erdős' minimum overlap problem, this was the best lower bound on mu when it appeared.

Source: https://arxiv.org/abs/2201.05704.

The retained PDF is arXiv:2201.05704v1 (27 pages), and the page numbers below are its PDF pages. The arXiv record (https://arxiv.org/abs/2201.05704, read 2026-10-02) names the Creative Commons Attribution 4.0 license.

Overview

White studies the minimum, over balanced partitions A⊔B=[2n]A\sqcup B=[2n], of the largest number of pairs (a,b)∈A×B(a,b)\in A\times B with a fixed difference a−ba-b (§1, pp. 1–2). The existence of the limit μ=lim⁡n→∞M(n)/n\mu=\lim_{n\to\infty}M(n)/n and its equality with the measurable function problem (1.1) (p. 2) are cited results of Haugland and Swinnerton-Dyer, respectively. Theorem 1 (p. 2) asserts μ≥0.379005\mu\ge 0.379005; the earlier lower and upper bounds quoted in §1 (pp. 1–2) are background results.

The method uses complementary functions f+g=1f+g=1 on [−1,1][-1,1] and their overlap M(x)=∫f(t)g(x+t) dtM(x)=\int f(t)g(x+t)\,dt (2.1) (§2, p. 2). Besides the mass identity (2.2) (p. 2), Lemma 6 (p. 8) gives the exact second moment ∫x2M(x) dx=2/3+E(M)2/2\int x^2M(x)\,dx=2/3+E(M)^2/2. Lemmas 2–3 (pp. 3–4) derive Fourier identities, including A2m≤0A_{2m}\le0 and B2m=0B_{2m}=0 in (3.5)–(3.6) (p. 5); Lemma 4 (p. 6) bounds the tails needed for finite truncation. Lemma 5 (§3.2, p. 7) bounds Fourier coefficients using interval averages of MM, and Lemma 7 (p. 9) relates those averages to its moments.

Section 4 (pp. 10–11) converts these conditions into a linear program. Proposition 8 (p. 10) applies its optimum to even overlap functions only; the section reports a verified numerical dual bound exceeding 0.3750.375 (p. 11). Section 5 (pp. 11–17) adds Fourier variables and quadratic constraints (5.1)–(5.13) (p. 12). Proposition 9 (p. 13) is the claimed link from an admissible function pair to this convex program. Tables 2–3 (pp. 16–17) and Figure 1 (p. 17) report dual bounds across parameter ranges; Appendix I (pp. 19–21) gives a second order cone formulation, while Appendix II (pp. 22–27) gives its dual, a floating point error check (8.4) (p. 24), and the certificate reuse formula in Lemma 10 (8.6) (p. 25). Section 6 (pp. 17–18) labels possible improvements and evenness of an optimizer as expectations, not theorems.

Two of the printed formulas are inconsistent with the lemmas they rest on; the printed factors and indices were checked on the page images of the retained arXiv:2201.05704v1 PDF. Constraints (5.6)–(5.7) (p. 12) carry the factor 8/(mπ)8/(m\pi) where (3.6) (p. 5) gives Bm=−4mπsin⁡(mπ/2) bmB_m=-\frac{4}{m\pi}\sin(m\pi/2)\,b_m, and the tail bounds (5.8)–(5.9) (p. 12) write mm in 4−m2/T24-m^2/T^2 and in the numerator for the variables ϵ2m−1,δ2m−1\epsilon_{2m-1},\delta_{2m-1}, which Proposition 9 (p. 13) defines as tails of the series at the odd index 2m−12m-1, so that Lemma 4 (p. 6) applied at that index gives a bound with 2m−12m-1 in both places. Proposition 9's feasibility argument (pp. 13–14) therefore does not follow literally as printed. This is the compilation's reading of the printed text, not a published erratum; Russell 2026 (Remark 9) records the same index slip in (5.8)/(5.9) independently. The full numerical dual assignments are also offered only upon request (§5.1, p. 16). The paper reports the numerical theorem but does not print a fully checkable certificate for it.

Relation to E36

This source bears on Problem 36.

In E36's notation, set rA,B(k)=∣{(a,b)∈A×B:a−b=k}∣r_{A,B}(k)=|\{(a,b)\in A\times B:a-b=k\}| and Q(n)=n−1min⁡A⊔B=[2n], ∣A∣=∣B∣=nmax⁡krA,B(k)Q(n)=n^{-1}\min_{A\sqcup B=[2n],\,|A|=|B|=n}\max_k r_{A,B}(k). Then Q(n)=M(n)/nQ(n)=M(n)/n in §1 (p. 1), and the cited limit and function correspondence (p. 2) identify lim⁡nQ(n)\lim_n Q(n) with White's μ\mu. Theorem 1's claimed conclusion (p. 2) is the lower bound lim inf⁡nQ(n)≥0.379005\liminf_n Q(n)\ge0.379005.

The usable route for a lower bound is to pass to (1.1) (p. 2), impose the mass and moment identities (2.2) (p. 2) and Lemma 6 (p. 8), then use the Fourier restrictions of Lemmas 2–5 (pp. 3–7) in a certified optimization bound. Proposition 8 (p. 10) supplies an argument only when MM is even; §6 (p. 17) explicitly treats evenness of an optimizer as an expectation. Proposition 9 (p. 13) and the dual construction in Appendices I–II (pp. 19–27) are intended to cover the general case, subject to the printed formula discrepancies noted above.

The paper gives no exact value of the E36 limit or matching construction. Its stated non-strict bound also does not by itself establish a strict improvement of the constant asked for by Problem 36, which would require some c>0.379005c>0.379005 with c≤lim inf⁡Q(n)c\le\liminf Q(n). The paper is relevant as a proposed quantitative lower-bound method, with its reported numerical conclusion requiring care when used as a proof from the printed text alone.

Bears on. #36

Results to transcribe.

  • Theorem 1: The minimum overlap constant mu satisfies mu >= 0.379005, improving Moser's bound sqrt(4 - sqrt 15) = 0.356394 and nearly matching Haugland's upper bound 0.3809268534330870.
  • Method: Elementary Fourier analysis on the continuous formulation M(x) = int f(t)g(x+t) dt yields linear constraints solved as a convex optimization program, with the bound improvable by more computation.
  • Baseline observation (2.2): M(x) has average value at least 0.25 on [-2,2], giving mu >= 0.25 as the elementary starting point.