arXiv:2608.04878v1

Quantitative Khintchine on the parabola with non-monotonic approximation functions

Maiken Gravgaard, Simon Kristensen

math.NT11J8311J13

Abstract

We prove a quantitative version of the convergence case of Khintchine's celebrated theorem in metric Diophantine approximation, but where the approximated points are restricted to lying on the parabola. A novel feature of our result is that unlike other results in literature, the approximating function is no longer required to be monotonic. This requires us to obtain explicit constants in classical number theoretic results, most notably in Burgess' bound for character sums in short intervals.

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Audit summary

Audited against arXiv v1

Not a correctness certificate. A “Correct” result may include yellow typos or minor formal corrections that do not affect substantive soundness. It means this audit found no unresolved substantive error under the stated criteria; it does not replace expert scrutiny or formal verification.

Current report

Detailed mathematical audit

Generated August 15, 2026
01Statements4 reported findingsContains unsupported statements

No counterexample was found to the four quantitative Khintchine statements. Their stated constants are nevertheless not verified: the common proof uses character-sum estimates outside the ranges actually established, and the quantitative lower-envelope reduction does not preserve the displayed dependence on the original approximation function. The restricted-denominator theorem has an additional scope ambiguity.

Theorems 4–5Not able to verify

The all-denominator and large-denominator constants are not established

Pages 2–3 and 7–15 · Theorems 4–5 and Sections 3.1–3.2 · arXiv:2608.04878v1

Both conclusions depend on Lemma 17 for every partial-sum length N=J/dN=J/d. In its small-modulus branch, however, the proof invokes Lemma 9, which is established only when q13/8Nq15/8q_1^{3/8}\leq N\leq q_1^{5/8}; neither the definition J=(6κψ(q))1J=\lfloor(6\kappa\psi(q))^{-1}\rfloor nor the theorem hypotheses impose this range. The proof also replaces ψ\psi by ψ~(q)=max{ψ(q),q5/8+η}\widetilde\psi(q)=\max\{\psi(q),q^{-5/8+\eta}\}, thereby increasing SψS_\psi and possibly maxψ\max\psi, but it continues to use the admissible bound for κ\kappa computed from the original quantities. These are genuine quantitative obligations, so the printed argument does not prove the displayed constants. They do not furnish a counterexample to either theorem.

Paper, version 1
Theorem 6Not able to verify

The restricted-prime-factor theorem is not verified in its printed scope

Pages 3 and 15–16 · Theorem 6 and Section 3.3 · arXiv:2608.04878v1

The proof begins with d(q)2nd(q)\leq2^n because qq has at most nn prime divisors. Under the standard reading that “prime divisors” means distinct prime divisors, this is false: q=2mq=2^m has one prime divisor but d(q)=m+1d(q)=m+1. The bound is valid if the hypothesis is instead Ω(q)k\Omega(q)\leq k (prime factors counted with multiplicity), or if qq is squarefree with at most kk prime factors. The theorem must state which restriction is intended and propagate it consistently. Independently, it inherits the Lemma 17 range gap and the quantitative lower-envelope gap from Theorem 4. No counterexample to the measure conclusion was found.

Paper, version 1
Theorem 7Not able to verify

The prime-denominator constant is not established for all admissible κ\kappa

Pages 3 and 16–17 · Theorem 7 and Section 3.4 · arXiv:2608.04878v1

The proof applies Lemma 12 to every partial sum ju(j/p)\sum_{j\leq u}(j/p) for 1uJ1\leq u\leq J. The cited bound is available only for interval length up5/8u\leq p^{5/8}, while the theorem permits arbitrarily small positive κ\kappa and hence arbitrarily large J=(6κψ(p))1J=\lfloor(6\kappa\psi(p))^{-1}\rfloor. Splitting off the multiples of pp does not put the remaining partial sums into the cited range; no estimate for the uncovered lengths is supplied. The theorem also inherits the unpreserved lower-envelope reduction. This prevents verification of the stated constant but does not disprove the conclusion.

McGown, Theorem 7.1 source
Theorems 4–7 · zero functionMinor formal correction

The identically zero approximation function needs a separate clause

Pages 2–3 · hypotheses and displayed bounds for κ(δ)\kappa(\delta) · arXiv:2608.04878v1

Each theorem allows ψ0\psi\equiv0, but its displayed bound then contains division by Sψ=0S_\psi=0 and by maxψ=0\max\psi=0. Add the assumption Sψ>0S_\psi>0, together with a separate sentence that ψ0\psi\equiv0 gives B(ψ,κ)=[0,1]\mathcal B'(\psi,\kappa)=[0,1] for every positive κ\kappa. This boundary repair is immediate and does not affect any nonzero approximation function.

02Proofs8 reported findingsContains incorrect or incomplete proofs

The proof does not justify the quantitative reduction to a power-law lower envelope, the small-modulus character estimate is used beyond its proved range and for a second character not checked by the supplied computation, and the prime proof likewise exceeds the cited Burgess range. The imprimitive-character passage is also incorrect as written. Several local formula and endpoint defects have verified repairs and are reported separately in yellow.

Section 3.1 · lower-envelope reductionIncomplete as written

Replacing ψ\psi changes the quantities that determine the advertised constant

Page 7 · first paragraph of Section 3.1; used throughout Sections 3.1–3.4 · arXiv:2608.04878v1

The inclusion B(ψ~,κ)B(ψ,κ)\mathcal B'(\widetilde\psi,\kappa)\subseteq\mathcal B'(\psi,\kappa) is correct, but it is insufficient for the quantitative theorem. The replacement ψ~(q)=max{ψ(q),q5/8+η}\widetilde\psi(q)=\max\{\psi(q),q^{-5/8+\eta}\} increases SψS_\psi and can increase maxψ\max\psi. The proof's final admissible bounds for κ\kappa are decreasing functions of those quantities, so a κ\kappa allowed by the theorem for the original ψ\psi need not satisfy the bound derived for ψ~\widetilde\psi. The coefficient-one lower bound is then used essentially to dominate three weighted series by SψS_\psi. Repair classification: No repair supplied; a quantitative approximation or a direct split of the small values of ψ\psi must preserve all constants. For Theorems 5–7 the replacement must also preserve their support restrictions.

Lemmas 9 and 17Incomplete as written

The small-modulus bound is applied for unproved lengths and an unchecked character

Pages 5, 9–12, and 17–19 · Lemma 9, Lemma 17, Equation (7), and Appendix A · arXiv:2608.04878v1

Lemma 9 is stated only for q3/8Nq5/8q^{3/8}\leq N\leq q^{5/8}, but Lemma 17 asserts its resulting Nq111/16\sqrt Nq_1^{11/16} estimate for every NN, and Equation (7) uses it at N=uN=u throughout 1uJ/d1\leq u\leq J/d. No argument treats u>q15/8u>q_1^{5/8}, which occurs for sufficiently small κ\kappa. Moreover, Appendix A computes only `kronecker_symbol(N,q)`, corresponding to (N/q)(N/q); it does not verify the separately stated character (q/N)(q/N) needed when q10(mod4)q_1\equiv0\pmod4. Repair classification: No repair supplied; the missing length ranges and the second character must be proved or exhaustively certified before Lemma 17 can support the main estimates.

Remark 11Incorrect as written

The imprimitive-character reduction is not a valid derivation as printed

Page 6 · Remark 11 and Equation (4) · arXiv:2608.04878v1

An induced character is printed as χ=χ1χ2\chi=\chi_1\chi_2 with primitive and principal moduli satisfying k1+k2=qk_1+k_2=q; no such additive modulus relation gives the displayed character identity. After writing n=utn=ut, the formula also silently replaces χ1(ut)\chi_1(ut) by χ(u)\chi(u) and omits the factor χ1(t)\chi_1(t). Absolute values can remove a nonzero factor χ1(t)\chi_1(t), but they do not justify replacing the primitive character by the original imprimitive one. Finally, the applicable Burgess estimate is governed by the conductor k1k_1, not merely by which numerical range contains qq. Repair classification: Plausible repair only. The standard conductor/radical decomposition can likely yield a divisor-factor loss, but its cases and constants must be written and propagated to Lemma 17.

Standard induced-character decomposition
Section 3.4 · prime character sumsIncomplete as written

McGown's interval-length hypothesis is not checked

Page 17 · application of Lemma 12 before the final measure estimate · arXiv:2608.04878v1

Lemma 12 provides the constant 10.036610.0366 only for lengths Np5/8N\leq p^{5/8}. Abel summation requires the bound for every uJu\leq J, but no inequality Jp5/8J\leq p^{5/8} follows from the hypotheses; indeed JJ grows without bound as κ\kappa decreases. Periodicity cancels complete periods, yet a remaining interval can still have length between p5/8p^{5/8} and pp5/8p-p^{5/8}, and the paper supplies no estimate there with the displayed constant. Repair classification: No repair supplied; an all-length estimate or a separate treatment of the remaining interval lengths is required.

McGown, Norm-Euclidean cyclic fields of prime degree
Theorem 6 · divisor countIncomplete as written

The proof needs prime factors counted with multiplicity

Page 15 · first sentence of Section 3.3 · arXiv:2608.04878v1

The estimate d(q)2nd(q)\leq2^n follows when qq is a product of at most nn primes counted with multiplicity: if q=piaiq=\prod p_i^{a_i} and ain\sum a_i\leq n, then d(q)=(ai+1)2aid(q)=\prod(a_i+1)\leq2^{\sum a_i}. It does not follow from having at most nn distinct prime divisors. The proof therefore verifies only the narrower interpretation and must state it explicitly. Repair classification: Verified conditional repair; replace the support hypothesis by Ω(q)k\Omega(q)\leq k (or impose squarefreeness with ω(q)k\omega(q)\leq k) and replace the stray nn by kk throughout.

Fejér kernelTypo

The closed form has an extra factor of two

Page 7 · display defining FJ\mathcal F_J and the following local estimate · arXiv:2608.04878v1

For the printed Fourier series, the correct identity is FJ(x)=1J2(sin(πJx)sin(πx))2,\mathcal F_J(x)=\frac1{J^2}\left(\frac{\sin(\pi Jx)}{\sin(\pi x)}\right)^2, not the displayed formula with 2πJx2\pi Jx and 2πx2\pi x. For example, at J=2,x=1/4J=2,x=1/4 the Fourier series equals 1/21/2 while the printed quotient equals 00. Replacing both occurrences of 2π2\pi by π\pi also makes the next local-sine argument valid and preserves the claimed lower bound 4/π24/\pi^2. The Fourier expansion determines this correction uniquely, so no subsequent constant changes.

Paper, version 1
Initial covering stepMinor formal correction

One scale factor and the endpoint representatives need correction

Page 7 · displays immediately preceding Equation (5) · arXiv:2608.04878v1

From qxa,qx2bκψ(q)|qx-a|,|qx^2-b|\leq\kappa\psi(q) one obtains a2/q2b/q3κψ(q)/q,\left|a^2/q^2-b/q\right|\leq3\kappa\psi(q)/q, so the displayed right side is missing `/q`; multiplying by qq then gives the correctly used condition a2/q3κψ(q)\|a^2/q\|\leq3\kappa\psi(q). Also, near x=0x=0 the nearest numerator can be a=0a=0, contrary to the printed 1aq1\leq a\leq q. Include a=0a=0 and pair the two endpoint half-intervals, or state their measure separately; because a=0a=0 and a=qa=q represent the same residue, their two half-lengths equal the one full interval already charged in Equation (5). These repairs are local and leave that measure bound unchanged.

Theorem 5 and Theorem 6 notationTypo

Several symbols have unique mechanical corrections

Pages 3, 14–15 · Theorem 6 and the Cauchy–Schwarz display in Section 3.2 · arXiv:2608.04878v1

In Theorem 6 and its proof, the undefined nn in 2n2^{-n} and 27n/22^{7n/2} should be the theorem's parameter kk. In the first Cauchy–Schwarz line on page 15, replace ψ(q)\sum\psi(q) by ψ(q)2\sum\psi(q)^2 and (r2t)2(r^2t)^2 by (r2t)2(r^2t)^{-2}; the immediately following line already uses exactly these corrected expressions. Finally, in the preceding Theorem 5 divisor split, the last nonsquare condition should cover all q1>105q_1>10^5; the constant 2727 dominates the large-range constant 55, and the subsequent displayed count is already over q1>105q_1>10^5. Each correction is forced by the adjacent formulas and changes no downstream estimate.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

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Paper
arXiv:2608.04878v1
Authors listed
Maiken Gravgaard, Simon Kristensen
Audit date
August 15, 2026
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