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Source. Liu--Sawhney, On further questions regarding unit fractions, arXiv:2404.07113v1, Fact 2.5, p. 8; see the source digest.

Statement, with the quadratic coefficient normalized. Define e(x)=exp⁡(2πix)e(x)=\exp(2\pi ix). Uniformly for ∣x∣≤1/2|x|\leq1/2 and q∈[0,1]q\in[0,1],

∣(1−q)+qe(x)−e(qx)(1−2π2q(1−q)x2)∣≪∣x∣3,(1)\left|(1-q)+qe(x) -e(qx)\bigl(1-2\pi^2q(1-q)x^2\bigr)\right| \ll |x|^3, \tag{1}

and

∣(1−q)+qe(x)∣≤1−8q(1−q)x2.(2)|(1-q)+qe(x)|\leq1-8q(1-q)x^2. \tag{2}

Source correction. The PDF prints 2π2\pi in (1), but the quadratic Taylor terms displayed in its own proof have coefficient 2π22\pi^2. With the stated normalization of ee, the coefficient in (1) must be 2π22\pi^2. Its displayed expansion of e(−qx)e(-qx) also has the wrong sign in the linear term. The proof below makes these local algebraic corrections explicit. The coefficient typo recurs in the proof of Lemma 3.1.

Proof. Multiply the Fourier factor by e(−qx)e(-qx), which has absolute value one. Taylor expansion with a uniform cubic remainder gives

(1−q)e(−qx)=(1−q)(1−2πiqx−2π2q2x2)+O(∣x∣3),qe((1−q)x)=q(1+2πi(1−q)x−2π2(1−q)2x2)+O(∣x∣3).\begin{aligned} (1-q)e(-qx) &=(1-q)\bigl(1-2\pi iqx-2\pi^2q^2x^2\bigr)+O(|x|^3),\\ qe((1-q)x) &=q\bigl(1+2\pi i(1-q)x -2\pi^2(1-q)^2x^2\bigr)+O(|x|^3). \end{aligned}

The constants add to one, the linear terms cancel, and the quadratic terms add to −2π2q(1−q)x2-2\pi^2q(1-q)x^2. This proves (1).

For (2), cos⁡(2πx)≤1−8x2\cos(2\pi x)\leq1-8x^2 on [−1/2,1/2][-1/2,1/2]. One way to check this elementary inequality is to use the concavity bound sin⁡(π∣x∣)≥2∣x∣\sin(\pi|x|)\geq2|x| and 1−cos⁡(2πx)=2sin⁡2(πx)1-\cos(2\pi x)=2\sin^2(\pi x). Consequently

∣(1−q)+qe(x)∣2=(1−q)2+q2+2q(1−q)cos⁡(2πx)≤1−16q(1−q)x2.\begin{aligned} |(1-q)+qe(x)|^2 &=(1-q)^2+q^2+2q(1-q)\cos(2\pi x)\\ &\leq1-16q(1-q)x^2. \end{aligned}

Here 0≤16q(1−q)x2≤10\leq16q(1-q)x^2\leq1. Applying 1−u≤1−u/2\sqrt{1-u}\leq1-u/2 proves (2).

Dependencies. Elementary Taylor expansion and trigonometric inequalities; no external theorem is invoked.

Bears on. #298 and #299, through the Fourier analysis in the quantitative reciprocal-sum criterion.