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Statement

Setting (pp. 1, 4). FF is the small-ball function of Theorem 1.1, F(δ)=P(sup⁡t≥0∣Yt∣≤δ)F(\delta)=\mathbb P(\sup_{t\ge0}\lvert Y_t\rvert\le\delta) with Yt=∫01e−ut dBuY_t=\int_0^1e^{-ut}\,dB_u (the paper's (2.1), p. 4).

Theorem 2.7 (p. 12). For δ∈(0,1/4)\delta\in(0,1/4),

log⁡F(δ)=−23π2log⁡3(1/δ)+O(log⁡5/2(1/δ)log⁡log⁡(1/δ)).\log F(\delta)=-\frac{2}{3\pi^2}\log^3(1/\delta)+O\Bigl(\log^{5/2}(1/\delta)\sqrt{\log\log(1/\delta)}\Bigr).

The paper presents it as the quantitative version of Theorem 1.2 (pp. 2, 12).

Source. Brayden Letwin and Mehtaab Sawhney, On the maxima of Littlewood polynomials on [−1,1][-1,1], arXiv:2604.19294v1 (2026). Labels and pages are those of arXiv v1: Theorem 2.7 on p. 12, its proof on pp. 12--13, the reductions it uses in Section 2 (pp. 4--12), Lemma 2.6 on p. 12 with its proof in Appendix A (pp. 24--29). The edition read is identified on the source card.

Read depth. Claims checked: the setting and the statement were read clause by clause on the printed pages. The proof was read but not checked step by step. Nothing here is independently reviewed.

Proof pointer

Pages 4--13 and 24--29. The substitution Zt=et/2YetZ_t=e^{t/2}Y_{e^t} and its stationary counterpart XtX_t, with covariance 12sech⁡((s−t)/2)\tfrac12\operatorname{sech}((s-t)/2) (the paper's (2.2)--(2.3), p. 4), reduce FF to G(δ)=P(sup⁡t≥0e−t/2∣Xt∣≤δ)G(\delta)=\mathbb P(\sup_{t\ge0}e^{-t/2}\lvert X_t\rvert\le\delta): for δ∈(0,1/4)\delta\in(0,1/4), exp⁡(−O(log⁡2(1/δ)))G(δ)≤F(δ)\exp(-O(\log^2(1/\delta)))G(\delta)\le F(\delta) and F(δ/2)G(1)exp⁡(−O(log⁡2(1/δ)log⁡log⁡(1/δ)))≪G(δ)F(\delta/2)G(1)\exp(-O(\log^2(1/\delta)\log\log(1/\delta)))\ll G(\delta) (Lemma 2.1, p. 4). The L∞L^\infty event for GG is then compared with the L2L^2 event H(δ)=P(∫0∞e−tXt2 dt≤δ2)H(\delta)=\mathbb P(\int_0^\infty e^{-t}X_t^2\,dt\le\delta^2) in both directions: by the Gaussian correlation inequality, G(δ)≤2H(4δlog⁡(1/δ))G(\delta)\le2H(4\delta\log(1/\delta)) (Lemma 2.3, p. 8), and by a local comparison with a smooth cutoff, H(δ)exp⁡(−O(log⁡2(1/δ)))≤G(Cδlog⁡4(1/δ))H(\delta)\exp(-O(\log^2(1/\delta)))\le G(C\delta\log^4(1/\delta)) (Lemmas 2.4 and 2.5, pp. 9--10). The L2L^2 asymptotic log⁡P(∫0∞e−tXt2 dt<δ)=−112π2log⁡3(1/δ)+O(log⁡5/2(1/δ)log⁡log⁡(1/δ))\log\mathbb P(\int_0^\infty e^{-t}X_t^2\,dt<\delta)=-\frac1{12\pi^2}\log^3(1/\delta)+O(\log^{5/2}(1/\delta)\sqrt{\log\log(1/\delta)}) (Lemma 2.6, p. 12), which the paper attributes in its o(⋅)o(\cdot) form to Nazarov and Petrova's survey, is proved in Appendix A by counting the eigenvalues of the covariance operator. Since the two comparison scales differ from δ\delta by polylogarithmic factors, the cubic main term carries over.

Dependencies

Royen's Gaussian correlation inequality; Anderson's inequality; Šidák's lemma (Lemma 2.1); Laptev's block decomposition and Karnik, Romberg and Davenport's eigenvalue bounds for prolate spheroidal wave functions (Appendix A).

Bears on

  • Problem 524: it implies Theorem 1.2, which the paper uses (Lemma 5.1, p. 18) to fix the constant (3π2/4)1/3(3\pi^2/4)^{1/3} in the logarithmic order of the lower envelope of Theorem 1.1; it does not mention the problem.