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Statement

For an irrational real number xx, the manuscript defines the irrationality exponent μ(x)\mu(x) as the supremum of the real ν>0\nu>0 for which 0<∣x−p/q∣<q−ν0<|x-p/q|<q^{-\nu} holds for infinitely many coprime integers p,qp,q with q≥2q\ge2; the pigeonhole principle gives μ(x)≥2\mu(x)\ge2 (p. 1).

Theorem 1.1. μ(π)=2\mu(\pi)=2. In the quantitative form the manuscript states: for every real ν>2\nu>2 there is an integer Q(ν)Q(\nu) such that

∣π−pq∣≥q−νfor all integers p and q with q≥Q(ν).\left|\pi-\frac pq\right|\ge q^{-\nu} \qquad\text{for all integers }p\text{ and }q\text{ with }q\ge Q(\nu).

The manuscript adds (p. 1) that the inequality holds for every integer numerator and denominator, whether or not the fraction is reduced; that Q(ν)Q(\nu) may depend on ν\nu and is not obtained effectively; and that exponent 22 is not the same as a uniform bound ∣π−p/q∣≥c/q2|\pi-p/q|\ge c/q^2, equivalently bounded continued-fraction partial quotients, which it does not claim. The proof concludes with the strict inequality for large qq, derives the irrationality of π\pi rather than assuming it, and states that no earlier irrationality bound for π\pi is used (pp. 4, 19).

Formalization. The release's Lean page for the family describes a formalization of this statement, with the comparator theorem OAI.PiExponent.main. In words, it says two things: for every real ν>2\nu>2 there is an integer Q≥2Q\ge2 with ∣π−p/q∣≥q−ν|\pi-p/q|\ge q^{-\nu} for all integers pp and all integers q≥Qq\ge Q; and the supremum of the set of ν>0\nu>0 for which infinitely many rationals rr with reduced denominator at least 22 satisfy 0<∣π−r∣<den⁡(r)−ν0<|\pi-r|<\operatorname{den}(r)^{-\nu} equals 22. The Lean page places the Flint–Hills consequence outside the formalized statement. It was read statically and not built or audited here, and the catalog lists no entry for it at this revision (see the card).

Source. OpenAI, The irrationality exponent of π\pi is 22, release folder preprints/The-irrationality-exponent-of-pi-is-2-September-24-2026; TeX file build/main.tex, label thm:main (lines 64--71), PDF p. 1, with the definition of μ\mu at lines 50--56 and the remark at lines 73--78; the proof closes at the end of Section 4 (build/sections/conclusion.tex, lines 55--156, PDF pp. 18--19). Provenance and attestations are on the card.

Read depth. Claims checked: the statement, the definition and the remark were read clause by clause in the TeX source, as were the statements of Theorem 2.1 (separated-weight interpolation), Proposition 3.4 (determinant comparison) and Lemma 4.1 (choice of constants). The proof in Sections 2--4 (pp. 4--19) was read for its structure only, as summarized below; no step was checked. Nothing here is independently reviewed.

Proof pointer

The proof is by contradiction. Fix ν>2\nu>2 and suppose that arbitrarily large denominators qq admit some pp with ∣π−p/q∣≤q−ν|\pi-p/q|\le q^{-\nu}. Write i\mathrm i for the imaginary unit.

Interpolation (Section 2, pp. 4--11). Theorem 2.1 is stated for arbitrary complex centers and does not involve π\pi. Given integers m,K≥1m,K\ge1 and positive rationals w0w_0, v0v_0 and θ<1\theta<1 with Kθm<1K\theta^m<1 and Kw0θm/v0<1Kw_0\theta^m/v_0<1, it chooses rational weights w1,…,wmw_1,\dots,w_m in turn, each above a threshold that depends on the fixed data and the earlier weights but not on the centers. Then at any KK points (1,cj1,…,cjm)(1,c_{j1},\dots,c_{jm}) whose iith coordinates are pairwise distinct for each ii, any choice of packets of Taylor coefficients in t,u1,…,umt,u_1,\dots,u_m of weight below HH (weights v0v_0 on tt and wi/θw_i/\theta on uiu_i), one at each point, is realized simultaneously by a single polynomial in Y,X1,…,XmY,X_1,\dots,X_m of weighted degree at most HH (weights w0,w1,…,wmw_0,w_1,\dots,w_m), expanded along Y=1+tY=1+t, Xi=cji+ui+log⁡(1+t)X_i=c_{ji}+u_i+\log(1+t); this holds for all large, suitably divisible HH. The key step is the curve inequality (Proposition 2.3): every irreducible curve meeting the affine chart has weighted degree at least 1+σ1+\sigma times its total weighted contact with these logarithmic curves at the centers. A violating curve would carry auxiliary polynomials with excess vanishing, whose derivatives along the commuting fields Y∂Y+∑i∂XiY\partial_Y+\sum_i\partial_{X_i} and ∂Xi\partial_{X_i} then vanish on it. A chain of derivative zero sets stabilizes on a component, where a weighted Bézout comparison of normal bases (Lemma 2.2) and the separation of the weights force dXi=dY/YdX_i=dY/Y; a residue argument shows this is impossible unless YY is constant, and the fiber Y=1Y=1 is excluded by a second auxiliary polynomial and the distinctness of coordinates. The curve inequality makes A−(1+σ)EA-(1+\sigma)E nef on the blowup of the jet ideal of the centers in a weighted projective compactification, so A−EA-E is ample and Serre vanishing gives surjectivity.

Two bounds for one determinant (Section 3, pp. 12--17). Choose mm of the assumed approximations pi/qip_i/q_i, set wi=⌈log⁡qi⌉w_i=\lceil\log q_i\rceil, and take the centers cji=2ijpi/qic_{ji}=2\mathrm ijp_i/q_i, 0≤j<K0\le j<K, rational approximations in Q(i)\mathbb Q(\mathrm i) to the periods 2πij2\pi\mathrm ij of the exponential function. After the logarithms are replaced by Taylor polynomials of length about F0wi/v0F_0w_i/v_0, Theorem 2.1 gives the interpolation matrix (columns the monomials of weighted degree at most HH, rows the Taylor coefficients at the centers) full row rank, so a square minor ΔH\Delta_H using every row is nonzero. Clearing the denominators, powers of the qiq_i and of lcm⁡(1,…,Ti−1)\operatorname{lcm}(1,\dots,T_i-1), gives a nonzero Gaussian integer and the lower bound of Lemma 3.1, log⁡∣ΔH∣/(MH)≥−(1−bˉ)−Ear\log|\Delta_H|/(MH)\ge-(1-\bar b)-E_{\mathrm{ar}}, where MM is the number of rows and bˉ\bar b their average normalized transverse weight. For the upper bound, Lemma 3.2 rewrites each row exactly, using e2πij=1e^{2\pi\mathrm ij}=1, as a combination of Taylor tests at z=2πij+log⁡(1+t)z=2\pi\mathrm ij+\log(1+t) of the entire functions fa,P(z)=[ua]P(ez,z+u1,…,z+um)f_{a,P}(z)=[u^a]P(e^z,z+u_1,\dots,z+u_m), with scalars carrying a factor e−νw⋅(a−β)e^{-\nu w\cdot(a-\beta)} from the approximation errors. Lemma 3.3 bounds any determinant of such tests: rows with the same transverse index aa test the same functions, so terms with a repeated Taylor degree cancel, and the rest give a factor exp⁡(−c∑ana2)\exp(-c\sum_an_a^2) with c=(log⁡2)/4c=(\log2)/4. Proposition 3.4 splits the expansion of ΔH\Delta_H: if at least a fraction η\eta of the rows have transverse weight at most AHAH, Cauchy–Schwarz over the few such indices gives a collision saving of order LL; otherwise the large indices give approximation-error factors of order ν(A(1−η)−bˉ)\nu(A(1-\eta)-\bar b). Either way the upper bound falls below Lemma 3.1 once g>0g>0, Ear+Ean<gE_{\mathrm{ar}}+E_{\mathrm{an}}<g and cL>1+Ear+EancL>1+E_{\mathrm{ar}}+E_{\mathrm{an}}, with g=ν(A(1−η)−θ)−(1−θ)g=\nu(A(1-\eta)-\theta)-(1-\theta).

Parameters (Section 4, pp. 17--19). Lemma 4.1 chooses rationals with θ<A<B<1<C\theta<A<B<1<C, ν(A−θ)>1−θ\nu(A-\theta)>1-\theta, B<1/CB<1/C and B<Cθ<1B<C\theta<1, by taking θ=1−δ\theta=1-\delta and A=1−bδA=1-b\delta with 1/2<b<1−1/ν1/2<b<1-1/\nu; such a bb exists exactly when ν>2\nu>2. On this page's reading, this is the one step that needs ν>2\nu>2: Section 3 states ν>2\nu>2 as a standing assumption, but its estimates use only ν≥1\nu\ge1. The proof fixes F0F_0, sets K=⌊Cm⌋K=\lfloor C^m\rfloor, w0=B−mw_0=B^{-m} and v0=2Kθmw0v_0=2K\theta^mw_0, and takes the dimension mm so large that the error terms depending on mm are small and cL>2cL>2, which is possible because LL grows like (B/A)m/m(B/A)^m/m. Only then does it pick the mm approximations, in turn, with denominators large enough for the weight thresholds of Theorem 2.1 and for the remaining error terms; since those thresholds do not depend on the centers, the choice is not circular. Proposition 3.4 then gives the contradiction as H→∞H\to\infty. The last paragraphs recover the irrationality of π\pi (exact representations would be approximations of every exponent) and the lower bound μ(π)≥2\mu(\pi)\ge2 by the pigeonhole principle.

Dependencies

External inputs, taken at statement level; none was checked here. The Bézout bound for isolated zeros of a complete intersection counted with local multiplicities (Mondal's notes, Corollary VIII.3 and Section IV.4.2); smooth projective models of curves, the standard properties of blowups and Rees algebras, and Serre vanishing (the Stacks Project, Tags 0BXX, 02OS, 02ND, 02NS, 0AG6, 0AG7 and 0B5U); and the criterion that nef plus ample is ample on a projective scheme (Lazarsfeld, Positivity in Algebraic Geometry I, Corollary 1.4.10). The cancellation of repeated Taylor degrees follows Laurent's interpolation determinants of exponential polynomials (Theorem 1 of his 2000 paper), applied within groups of rows, and the bound log⁡lcm⁡(1,…,n)≤4nlog⁡2\log\operatorname{lcm}(1,\dots,n)\le4n\log2 is proved in the text. The earlier upper bounds for μ(π)\mu(\pi) that the introduction surveys are not inputs.

Bears on

No problem page is identified as using this result; the card's Bears on section records the pages read for a possible use.