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Lemma (p. 2, §2.3, unnumbered). For x>0x>0 and integers 2≤m≤n2\le m\le n,

∏i=1ncosh⁡(x/i)≤(1+e−2x/m2)mexp⁡(xHm+x22m).(1)\prod_{i=1}^n\cosh(x/i) \le \left(\frac{1+e^{-2x/m}}2\right)^m \exp\left(xH_m+\frac{x^2}{2m}\right). \tag{1}

The source's Lemma is (1) alone. The elementary quadratic estimate used in its proof also gives the following comparison, which is not part of the Lemma: for n≥1n\ge1 and t>0t>0,

P(Zn≥t)≤exp⁡(−t22Vn).(2)\mathbb P(Z_n\ge t)\le\exp\left(-\frac{t^2}{2V_n}\right). \tag{2}

At t=Hn−2>0t=H_n-2>0, the logarithm of the right side of (2), divided by nn, tends to zero. Thus that bound alone does not give the exponential saving in the main theorem.

Proof. For i≤mi\le m, the inequality x/i≥x/mx/i\ge x/m gives

cosh⁡(x/i)=ex/i1+e−2x/i2≤ex/i1+e−2x/m2.\cosh(x/i) =e^{x/i}\frac{1+e^{-2x/i}}2 \le e^{x/i}\frac{1+e^{-2x/m}}2.

Multiplying these first mm inequalities yields

∏i=1mcosh⁡(x/i)≤exHm(1+e−2x/m2)m.(3)\prod_{i=1}^m\cosh(x/i) \le e^{xH_m}\left(\frac{1+e^{-2x/m}}2\right)^m. \tag{3}

For every real yy,

cosh⁡y=∑k=0∞y2k(2k)!≤∑k=0∞y2k2kk!=ey2/2.(4)\cosh y =\sum_{k=0}^\infty\frac{y^{2k}}{(2k)!} \le\sum_{k=0}^\infty\frac{y^{2k}}{2^k k!} =e^{y^2/2}. \tag{4}

Indeed, (2k)!=∏j=1k(2j)(2j−1)≥∏j=1k2j=2kk!(2k)!=\prod_{j=1}^k(2j)(2j-1)\ge\prod_{j=1}^k2j=2^k k!, and all displayed series terms are nonnegative. Therefore

∏i=m+1ncosh⁡(x/i)≤exp⁡(x22∑i=m+1n1i2)≤exp⁡(x22m).(5)\prod_{i=m+1}^n\cosh(x/i) \le\exp\left(\frac{x^2}{2}\sum_{i=m+1}^n\frac1{i^2}\right) \le\exp\left(\frac{x^2}{2m}\right). \tag{5}

The last step follows from

∑i=m+1n1i2≤∑i=m+1∞1i2≤∫m∞duu2=1m.\sum_{i=m+1}^n\frac1{i^2} \le\sum_{i=m+1}^\infty\frac1{i^2} \le\int_m^\infty\frac{du}{u^2}=\frac1m.

When m=nm=n, the product in (5) is the empty product, equal to one, and its bound still holds. Combining (3) and (5) proves (1).

To verify the comparison (2), apply (4) to every factor in the exponential-moment bound:

P(Zn≥t)≤exp⁡(−xt+x2Vn/2).\mathbb P(Z_n\ge t) \le\exp(-xt+x^2V_n/2).

Since Vn>0V_n>0, the permitted choice x=t/Vnx=t/V_n proves (2). Also

1≤Vn≤1+∫1∞u−2 du=2,log⁡(n+1)≤Hn≤1+log⁡n.1\le V_n\le1+\int_1^\infty u^{-2}\,du=2, \qquad \log(n+1)\le H_n\le1+\log n.

The harmonic bounds follow by comparing the decreasing function 1/u1/u with its sums on the adjacent unit intervals. Hence Hn−2H_n-2 tends to infinity and is O(log⁡n)O(\log n), while Vn≥1V_n\ge1. It follows that

1nlog⁡(exp⁡(−(Hn−2)22Vn))⟶0.\frac1n\log\left(\exp\left(-\frac{(H_n-2)^2}{2V_n}\right)\right) \longrightarrow0.

For any fixed b>0b>0, the right side of (2) at this value of tt is therefore larger than e−bne^{-bn} for all sufficiently large nn. This is a limitation of that estimate, not a lower bound on the actual tail probability. □\square

Source. Steinerberger, arXiv:2403.17041v5, unnumbered Lemma, p. 2, §2.3; proof on p. 3. The final comparison expands the explanation in §2.2. The proof uses the elementary bound Vn≤2V_n\le2; the source's sharper π2/6\pi^2/6 bound is unnecessary.

Read depth. Claims checked: the statement of (1), with x>0x>0 and 2≤m≤n2\le m\le n, was read on p. 2, and the source's proof on p. 3. The proof above is written here along that route and is not recorded as independently verified.

Bears on. #297 only through the Theorem, whose proof uses it.