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Wang: A Proposed Solution to Erdős Problem 486

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Shouqiao Wang, "A Proposed Solution to Erdős Problem 486," preprint, 2026. Source: https://github.com/ShouqiaoW/erdos/tree/main/486. The retained folder-name PDF is the 10-page preprint from that repository; its version date and retrieval date are not recorded. A Markdown reading copy sits beside it. The file prints no notice of its own on pp. 1--2 or 9--10; the repository holding it, whose folder 486 holds this preprint, carries a LICENSE file that GitHub shows as "MIT license", the MIT License for the repository as a whole (https://github.com/ShouqiaoW/erdos, read 2026-10-02), and whether the author meant it to cover the manuscript text is not stated. The abstract presents the manuscript as a proposed solution and says that GPT-5.6 found it.

Overview

Wang studies the delayed multi-residue sieve obtained from an arbitrary set of moduli A⊆NA\subseteq\mathbb N and subsets Xn⊆Z/nZX_n\subseteq\mathbb Z/n\mathbb Z:

B(A,X)={m∈N:m mod n∉Xn for every n∈A with n<m}.B(A,X)=\{m\in\mathbb N:m\bmod n\notin X_n\text{ for every }n\in A\text{ with }n<m\}.

This is equation (1.1) in Section 1. The question is whether LB(x)=(log⁡x)−1∑m<x, m∈Bm−1L_B(x)=(\log x)^{-1}\sum_{m<x,\,m\in B}m^{-1} must converge. Theorem 1.1 gives a negative answer: there are fixed infinite AA and fixed sets XnX_n for which

lim inf⁡x→∞LB(x)≤177/200<49/50≤lim sup⁡x→∞LB(x).\liminf_{x\to\infty}L_B(x)\le 177/200<49/50\le\limsup_{x\to\infty}L_B(x).

The result is a counterexample to Problem 486. The manuscript attributes the original formulation to Erdős [7, p. 48] and [8, pp. 235--236].

The proof combines finite probabilistic deletion blocks with a deterministic gliding-hump construction. Lemma 2.1 in Section 2 is the recovery mechanism: for any finite family F={(q,Yq)}\mathcal F=\{(q,Y_q)\}, if UF⊂Z^U_{\mathcal F}\subset\widehat{\mathbb Z} is the union of the associated residue cylinders, then

∑m<x, m∈BF1m=(1−μ(UF))log⁡x+OF(1).\sum_{m<x,\,m\in B_{\mathcal F}}\frac1m =(1-\mu(U_{\mathcal F}))\log x+O_{\mathcal F}(1).

The proof reduces the eventual survivor set to a union of residue classes modulo the least common multiple of the finitely many moduli. Remark 1.2 shows that replacing the strict activation condition q<mq<m by the inclusive condition q≤mq\le m changes the survivor set by a primitive set and hence by logarithmic weight o(log⁡x)o(\log x), using Behrend [3, pp. 42--44].

Section 3 constructs one block at the dyadic scale Q=2jQ=2^j. Lemma 3.1 associates distinct moduli qSq_S to central subsets S⊆{1,…,k}S\subseteq\{1,\ldots,k\}, where k=2⌊j/8⌋k=2\lfloor\sqrt j/8\rfloor, so that

19Q/20≤qS≤21Q/20,pi∣qS⟺i∈S,(3.1)19Q/20\le q_S\le21Q/20, \qquad p_i\mid q_S\Longleftrightarrow i\in S, \tag{3.1}

and every point of J=[11Q/10,19Q/10]∩ZJ=[11Q/10,19Q/10]\cap\mathbb Z lies in (qS,2qS](q_S,2q_S]. Independent Bernoulli labels modulo the auxiliary primes define K(m)K(m) and select endpoints E={m∈J:K(m)∈Sk}E=\{m\in J:K(m)\in\mathcal S_k\}, assigning qm=qK(m)q_m=q_{K(m)}. Lemma 3.2, by McDiarmid's bounded-differences inequality, gives

P(∣E∣<∣J∣/2)≤exp⁡(−4k/(8k)).\mathbb P(|E|<|J|/2)\le \exp(-4^k/(8k)).

Lemma 3.3 proves that the completed periodic footprint U=⋃m∈E[m]qmU=\bigcup_{m\in E}[m]_{q_m} satisfies

P(μ(U)>e−k/100)≤3e−k/100.\mathbb P(\mu(U)>e^{-k/100})\le3e^{-k/100}.

Its main ingredients are the candidate characterization (3.2), the collision estimate (3.3), the one-candidate probability (3.4), Hoeffding's tail bound (3.5), and the entropy and candidate-count estimates (3.6) and (3.7). These are probabilistic existence arguments; no explicit labels or blocks are computed.

Lemma 3.4 extracts a deterministic block: for every sufficiently large jj, there are Ej⊂[11Q/10,19Q/10]E_j\subset[11Q/10,19Q/10], assigned moduli qj,m<mq_{j,m}<m, and a cylinder union UjU_j such that

∣Ej∣≥3Q/8,19Q/20≤qj,m≤21Q/20,μ(Uj)≤ηj=e−kj/100,(3.8)|E_j|\ge3Q/8,\qquad 19Q/20\le q_{j,m}\le21Q/20, \qquad \mu(U_j)\le\eta_j=e^{-k_j/100}, \tag{3.8}

with ∑jηj<∞\sum_j\eta_j<\infty. Thus the active classes delete a fixed amount of local harmonic mass while their eventual periodic union has summably small Haar measure.

Section 4 assembles blocks in epochs It={at,…,2at}I_t=\{a_t,\ldots,2a_t\}. The tail bounds in (4.1) keep the accumulated periodic footprint below ϵ=1/100\epsilon=1/100. Lemma 2.1 permits the next epoch to be delayed until the finite past has recovered: at xt=2at−1x_t=2^{a_t-1}, equation (4.2) gives a finite-past average at least 49/5049/50. Every modulus from epoch tt or later exceeds xtx_t, so it is inactive below xtx_t, and the scale-separation inequality (4.3) keeps later scales from adding classes to earlier moduli; this gives the limsup bound (4.4). Conversely, all endpoints in epoch tt have been deleted by yt=22at+1y_t=2^{2a_t+1}. Their harmonic contribution is bounded below scale by scale, yielding (4.5) and the liminf bound (4.6). These two subsequences prove Theorem 1.1.

The construction lies outside the known positive regimes. Section 1 cites the Davenport--Erdős theorem for the zero-residue case [5, pp. 147--151], its later elementary proof [6, pp. 19--24], Besicovitch's failure of natural density [2, pp. 336--341], and Araújo's summable multi-residue result [1, Theorem 3.25]. Remark 4.1 proves for Wang's system that every installed scale contributes at least 5/145/14 to ∑q∈A∣Xq∣/q\sum_{q\in A}|X_q|/q, so that series diverges.

Relation to E25

This source bears on Problem 25.

Enumerate Wang's modulus set increasingly as n1<n2<⋯n_1<n_2<\cdots. E25 corresponds to imposing

Xni={ai mod ni}X_{n_i}=\{a_i\bmod n_i\}

for every ii. Apart from activation at equality, its uncovered set is then Wang's B(A,X)B(A,X): E25 tests the congruence when n=nin=n_i, whereas equation (1.1) activates a modulus only when ni<nn_i<n. Remark 1.2 proves that these strict and inclusive conventions have the same logarithmic-density behavior, since their difference has harmonic sum o(log⁡x)o(\log x). Activation convention is therefore not the obstruction to transferring the counterexample.

Several components are directly usable for E25. Lemma 2.1 applies verbatim to a finite singleton system Yni={ai}Y_{n_i}=\{a_i\}, identifying its recovered logarithmic density with

1−μ ⁣(⋃i[ai]ni).1-\mu\!\left(\bigcup_i[a_i]_{n_i}\right).

Sections 4.1 and 4.3 then give a general gliding-hump principle: after finitely many singleton classes have recovered, later moduli can be placed above the chosen cutoff and are inactive below it. Likewise, the deletion argument of Section 4.4 would transfer if one could construct singleton blocks having (i) a fixed positive local harmonic deletion, (ii) summably small completed periodic footprints, (iii) moduli below their deleted endpoints, and (iv) separation between scales.

The paper does not supply such singleton blocks; Section 5 states that the argument does not settle Problem 25. In Lemma 3.4, qj,m=qK(m)q_{j,m}=q_{K(m)}, so all endpoints with the same label set K(m)=SK(m)=S use the same modulus and become distinct elements of the multi-residue set XqSX_{q_S}. There are at most ∣Sk∣≤2k=exp⁡(O(j))|\mathcal S_k|\le2^k=\exp(O(\sqrt j)) available moduli at scale jj, while ∣Ej∣≥3⋅2j/8|E_j|\ge3\cdot2^j/8. Retaining at most one endpoint per modulus would therefore leave only exp⁡(O(j))\exp(O(\sqrt j)) endpoints of size ≍2j\asymp2^j, losing the fixed harmonic deletion required in (4.5). Remark 4.1 also explicitly counts the many residue classes through ∣Xq∣|X_q|. No argument is given for replacing repeated uses of qSq_S by distinct moduli while preserving the small-footprint estimate of Lemma 3.3.

Consequently, Theorem 1.1 is a counterexample only for the multi-residue generalization. Its concrete contribution to E25 is the recovery-and-epoch framework and a sharply identified missing ingredient: a singleton analogue of the finite block in Lemma 3.4.