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Statement

For a set EE of positive integers, write R(E)=∑n∈E1/nR(E)=\sum_{n\in E}1/n, Ed={n∈E:d∣n}E_d=\{n\in E:d\mid n\}, and QE={pa:pa∣n for some n∈E, a≥1}\mathcal Q_E=\{p^a:p^a\mid n\text{ for some }n\in E,\ a\ge1\}. Brackets denote least common multiples, and Q=[QA]=lcm⁡(A)Q=[\mathcal Q_A]=\operatorname{lcm}(A). An integer is SS-smooth in this paper when every prime-power divisor, not just every prime divisor, is at most SS. Put e(u)=exp⁡(2πiu)e(u)=\exp(2\pi iu).

There is an absolute constant C≥1C\ge1 with the following property. Fix δ∈(0,1)\delta\in(0,1) and ε∈(0,1/10)\varepsilon\in(0,1/10), and take NN sufficiently large in terms of these two parameters. Suppose η≥(log⁡N)−1\eta\ge(\log N)^{-1} and

N0.99≤S≤K≤M≤N/104.N^{0.99}\le S\le K\le M\le N/10^4.

Define

Γ=max⁡{η(log⁡N)δ(log⁡log⁡N)3,η2(log⁡N)1−2δlog⁡2(N/M)(log⁡log⁡N)5}.\Gamma=\max\left\{ \frac{\eta}{(\log N)^\delta(\log\log N)^3}, \frac{\eta^2(\log N)^{1-2\delta}} {\log^2(N/M)(\log\log N)^5}\right\}.

Assume also

S≤min⁡{M2CN,ηMK2N2(log⁡N)3},K≤Mexp⁡(−(log⁡N)1−δ),S\le\min\left\{\frac{M^2}{CN},\frac{\eta MK^2}{N^2(\log N)^3}\right\}, \qquad K\le M\exp(- (\log N)^{1-\delta}),

and

C≤Γ2(log⁡N)2ε(log⁡(N/M)+(log⁡N)1−δ).C\le\frac{\Gamma^2} {(\log N)^{2\varepsilon}(\log(N/M)+(\log N)^{1-\delta})}.

Let A⊆[M,N]A\subseteq[M,N] satisfy

  • every n∈An\in A is SS-smooth;
  • Ω(n)≤5log⁡log⁡N\Omega(n)\le5\log\log N for every n∈An\in A;
  • min⁡q∈QAqR(Aq)≥η\min_{q\in\mathcal Q_A}qR(A_q)\ge\eta.

If xx is a positive integer and

(1+(log⁡N)−1)xQ≤R(A)≤(log⁡N)xQ,(1+(\log N)^{-1})\frac xQ\le R(A)\le(\log N)\frac xQ,

there is B⊆AB\subseteq A such that R(B)=x/QR(B)=x/Q.

Source: Liu–Sawhney, arXiv:2404.07113v1, Proposition 5.2, printed/PDF pp. 16–19 (the statement is on p. 16 and the last proof estimate is on p. 19). The source uses the first term in Γ\Gamma for Theorem 1.1 and the second for Theorem 1.3 and Proposition 1.4.

Rewritten proof

The proof follows pp. 16–19 with explicit corrections to the residue notation, Fourier threshold, dyadic endpoints and parameter estimates. It uses the proved application form of Lemma 5.1, rather than its false unrestricted statement as printed. The corrections are recorded below; none is attributed to an author erratum or to the uninspected published version.

Feasible parameters and the divisor scale

Write

L=log⁡N,ℓ=log⁡log⁡N,w=log⁡(N/M),a=L1−δ.L=\log N,\quad\ell=\log\log N,\quad w=\log(N/M), \quad a=L^{1-\delta}.

The hypotheses give log⁡104≤w≤.01L\log10^4\le w\le.01L. The positive mass condition makes AA nonempty. For any q∈QAq\in\mathcal Q_A, we have q≤S≤Me−aq\le S\le Me^{-a}, so harmonic summation gives

η≤qR(Aq)≤∑M/q≤m≤N/q1m≤w+O(q/M)≤2w.\eta\le qR(A_q) \le\sum_{M/q\le m\le N/q}\frac1m \le w+O(q/M)\le2w.

Let Γ1,Γ2\Gamma_1,\Gamma_2 denote the two terms in Γ\Gamma. If δ≥1/2\delta\ge1/2, then

Γ12L2ε(w+a)≤4wL2δ+2εℓ6→0,Γ22L2ε(w+a)≤16L2−4δ−2εℓ10(w+a)→0.\frac{\Gamma_1^2}{L^{2\varepsilon}(w+a)} \le\frac{4w}{L^{2\delta+2\varepsilon}\ell^6}\to0, \qquad \frac{\Gamma_2^2}{L^{2\varepsilon}(w+a)} \le\frac{16L^{2-4\delta-2\varepsilon}}{\ell^{10}(w+a)}\to0.

This contradicts the last hypothesis. Thus every feasible fixed choice has δ<1/2\delta<1/2. In particular,

Γ≫Lεa=Lε+(1−δ)/2≫L3ε,\Gamma\gg L^\varepsilon\sqrt a =L^{\varepsilon+(1-\delta)/2}\gg L^{3\varepsilon},

since ε<1/10\varepsilon<1/10. The divisor lemma will be applied with mass parameter η/2\eta/2. Its scale is therefore

H∗=eρ,ρ=ηa2ℓ3w,Γ=max⁡{2ρwL,4ρ2ℓL}.H_*=e^\rho,\qquad\rho=\frac{\eta a}{2\ell^3w},\qquad \Gamma=\max\left\{\frac{2\rho w}{L}, \frac{4\rho^2\ell}{L}\right\}.

The final hypothesis forces Γ→∞\Gamma\to\infty. A bounded subsequence of ρ\rho would make both expressions on the right bounded, so ρ→∞\rho\to\infty. Thus H∗≥2H_*\ge2 for large NN, as required by the corrected application form of Lemma 5.1.

Fourier reduction and concentration

Set

τ=x/QR(A),1log⁡N≤τ≤log⁡N1+log⁡N.\tau=\frac{x/Q}{R(A)},\qquad \frac1{\log N}\le\tau\le\frac{\log N}{1+\log N}.

Include each n∈An\in A independently in BB with probability τ\tau. Integer Fourier orthogonality gives

P(R(B)−x/Q∈Z)=∑B⊆Aτ∣B∣(1−τ)∣A∖B∣1Q∑−Q/2<h≤Q/2e ⁣(∑n∈Bhn−hxQ)=1Q∑−Q/2<h≤Q/2e(−hx/Q)∏n∈A(1−τ+τe(h/n))=1Q∑−Q/2<h≤Q/2Re⁡ ⁣(e(−hx/Q)∏n∈A(1−τ+τe(h/n))).(5.1–5.2)\begin{aligned} \mathbb P(R(B)-x/Q\in\mathbb Z) &=\sum_{B\subseteq A}\tau^{|B|}(1-\tau)^{|A\setminus B|} \frac1Q\sum_{-Q/2<h\le Q/2} e\!\left(\sum_{n\in B}\frac hn-\frac{hx}Q\right)\\ &=\frac1Q\sum_{-Q/2<h\le Q/2} e(-hx/Q)\prod_{n\in A}(1-\tau+\tau e(h/n))\\ &=\frac1Q\sum_{-Q/2<h\le Q/2} \operatorname{Re}\!\left(e(-hx/Q) \prod_{n\in A}(1-\tau+\tau e(h/n))\right). \end{aligned} \tag{5.1–5.2}

The last equality also follows by conjugate symmetry. It will suffice to show that this probability is at least 1/(2Q)1/(2Q) and that the probability of a nonzero integer discrepancy is less than 1/(4Q)1/(4Q). Since ER(B)=x/Q\mathbb ER(B)=x/Q and each summand changes by at most 1/M1/M, Lemma 2.6 gives

P(∣R(B)−x/Q∣≥1)≤2exp⁡(−M2/(2N)).\mathbb P(|R(B)-x/Q|\ge1) \le2\exp(-M^2/(2N)).

By smoothness and Theorem 2.1, Q≤∏q≤Sq≪e5SQ\le\prod_{q\le S}q\ll e^{5S}. The condition S≤M2/(CN)S\le M^2/(CN), with CC large, implies 2exp⁡(−M2/(2N))≤e−6S<1/(4Q)2\exp(-M^2/(2N))\le e^{-6S}<1/(4Q) for sufficiently large NN.

Major arcs

We first justify the cardinality needed by Lemma 3.1. Put y0=ea/(10ℓ)y_0=e^{a/(10\ell)}, and let p0p_0 be the smallest prime dividing an element of AA. If p0≥y0p_0\ge y_0, each n/p0n/p_0 with n∈Ap0n\in A_{p_0} avoids every prime below y0y_0. Furthermore M/p0≥M/S≥eaM/p_0\ge M/S\ge e^a. Lemma 2.4 applied to doubling intervals, followed by reciprocal summation across O(w)O(w) such intervals, gives

η≤p0R(Ap0)≪wlog⁡y0=10wℓa.\eta\le p_0R(A_{p_0})\ll\frac w{\log y_0} =\frac{10w\ell}{a}.

The sieve cutoff holds because the local logarithmic scale is at least a+O(1)a+O(1) and its second logarithm is at most ℓ+o(1)\ell+o(1). The displayed bound contradicts η=2ρℓ3w/a\eta=2\rho\ell^3w/a and ρ→∞\rho\to\infty. Hence p0<y0p_0<y_0, and

∣A∣≥MR(Ap0)≥ηMp0≥MLy0≥N.99−o(1)>N.95.|A|\ge M R(A_{p_0})\ge\frac{\eta M}{p_0} \ge\frac M{Ly_0}\ge N^{.99-o(1)}>N^{.95}.

We may therefore apply Lemma 3.1 with all inclusion probabilities equal to τ\tau, obtaining

1Q∑∣h∣≤M/2Re⁡ ⁣(e(−hx/Q)∏n∈A(1−τ+τe(h/n)))≥34Q.\frac1Q\sum_{|h|\le M/2} \operatorname{Re}\!\left(e(-hx/Q) \prod_{n\in A}(1-\tau+\tau e(h/n))\right)\ge\frac3{4Q}.

The allowed interval for τ\tau is inside [(log⁡N)−2,1−(log⁡N)−2][(\log N)^{-2},1-(\log N)^{-2}] for large NN, as required by Lemma 3.1.

Minor arcs: decay

For each nn, let hn∈(−n/2,n/2]h_n\in(-n/2,n/2] be the integer congruent to hh modulo nn, and put

t=50N2Lℓτ(1−τ)K2,Ih=(h−K/2,h+K/2).t=\frac{50N^2L\ell}{\tau(1-\tau)K^2},\qquad I_h=(h-K/2,h+K/2).

Define the exceptional prime powers by

Dh={q∈QA:∣{n∈Aq:∣hn∣≥K/2}∣<t}.\mathcal D_h=\left\{q\in\mathcal Q_A: |\{n\in A_q:|h_n|\ge K/2\}|<t\right\}.

Each nn belongs to at most Ω(n)≤5log⁡log⁡N\Omega(n)\le5\log\log N of the sets AqA_q. Applying Fact 2.5 gives

(∏n∈A∣1−τ+τe(h/n)∣)5log⁡log⁡N≤∏q∈QA∏n∈Aq∣1−τ+τe(h/n)∣≤∏q∈QA∖Dhexp⁡(−2τ(1−τ)K2t/N2)≤exp⁡(−100∣QA∖Dh∣log⁡Nlog⁡log⁡N).\begin{aligned} \left(\prod_{n\in A}|1-\tau+\tau e(h/n)|\right)^{5\log\log N} &\le\prod_{q\in\mathcal Q_A}\prod_{n\in A_q} |1-\tau+\tau e(h/n)|\\ &\le\prod_{q\in\mathcal Q_A\setminus\mathcal D_h} \exp(-2\tau(1-\tau)K^2t/N^2)\\ &\le\exp(-100|\mathcal Q_A\setminus\mathcal D_h| \log N\log\log N). \end{aligned}

Taking the 1/(5ℓ)1/(5\ell) power gives N−20N^{-20} per exceptional complement element, and in particular

∏n∈A∣1−τ+τe(h/n)∣≤N−10∣QA∖Dh∣.(5.3)\prod_{n\in A}|1-\tau+\tau e(h/n)| \le N^{-10|\mathcal Q_A\setminus\mathcal D_h|}. \tag{5.3}

For each large-residue factor we used ∣1−τ+τe(h/n)∣≤exp⁡(−2τ(1−τ)K2/N2)|1-\tau+\tau e(h/n)|\le\exp(-2\tau(1-\tau)K^2/N^2).

Minor arcs: a common multiple near h

For q∈Dhq\in\mathcal D_h let

Tq={n∈Aq:∣hn∣<K/2}.T_q=\{n\in A_q:|h_n|<K/2\}.

With the definition of Dh\mathcal D_h, ∣Aq∖Tq∣<t|A_q\setminus T_q|<t and

R(Tq)≥R(Aq)−t/M≥η/q−t/M≥η/(2q).R(T_q)\ge R(A_q)-t/M\ge\eta/q-t/M\ge\eta/(2q).

Indeed, τ(1−τ)≥1/(2L)\tau(1-\tau)\ge1/(2L) for the allowed probability range, so the stated bound on SS gives

tM≤100N2L2ℓMK2≤η2S\frac tM\le\frac{100N^2L^2\ell}{MK^2} \le\frac\eta{2S}

for large NN, since L≥200ℓL\ge200\ell eventually. Apply the corrected application form of Lemma 5.1 to TqT_q with mass parameter η/2\eta/2, obtaining dqd_q and Tq∗⊆(Tq)qdqT_q^*\subseteq(T_q)_{qd_q}. Its global prime-factor bound is inherited from AA; we already proved δ<1/2\delta<1/2 and H∗≥2H_*\ge2. The size condition for qq follows from q≤S≤K≤Mexp⁡(−(log⁡N)1−δ)q\le S\le K\le M\exp(- (\log N)^{1-\delta}). It gives

qdq≥Mexp⁡(−(log⁡N)1−δ)≥K.qd_q\ge M\exp(- (\log N)^{1-\delta})\ge K.

There is at most one multiple of qdqqd_q in IhI_h. Since a nonempty Tq∗T_q^* consists of integers with a multiple in IhI_h, there is such a multiple; call it xqx_q. Put

T~q={n/(qdq):n∈Tq∗}.\widetilde T_q=\{n/(qd_q):n\in T_q^*\}.

The reciprocal-mass conclusion gives

R(T~q)=qdqR(Tq∗)≥ηC(log⁡N)δlog⁡log⁡N.R(\widetilde T_q)=qd_qR(T_q^*) \ge\frac\eta{C(\log N)^\delta\log\log N}.

The same output gives min⁡T~q≥H∗\min\widetilde T_q\ge H_* and max⁡T~q/min⁡T~q≤ew\max\widetilde T_q/\min\widetilde T_q\le e^w. Put E=T~qE=\widetilde T_q and use all dyadic bins [2j,2j+1)[2^j,2^{j+1}) with

⌊log⁡2min⁡E⌋≤j≤⌊log⁡2max⁡E⌋.\lfloor\log_2\min E\rfloor\le j\le\lfloor\log_2\max E\rfloor.

This includes the bin containing the minimum. Because ρ→∞\rho\to\infty, the indices are large and positive. Their reciprocal weights satisfy

W:=∑j1j+1≪min⁡{ℓ,w+1ρ}≪min⁡{ℓ,2w2ℓ3ηa}.W:=\sum_j\frac1{j+1} \ll\min\left\{\ell,\frac{w+1}{\rho}\right\} \ll\min\left\{\ell,\frac{2w^2\ell^3}{\eta a}\right\}.

The first estimate follows either by summing 1/(j+1)1/(j+1) up to O(L)O(L) or by bounding the number of bins by O(w+1)O(w+1) and the smallest index below by a constant times ρ\rho. The second uses w≥log⁡104w\ge\log10^4. Since the bins partition EE,

R(E)≤Wmax⁡j((j+1)R(E∩[2j,2j+1))).R(E)\le W\max_j\bigl((j+1)R(E\cap[2^j,2^{j+1}))\bigr).

Thus some yq=2jy_q=2^j has

R(E∩[yq,2yq))≥clog⁡yqmax⁡{ηLδℓ2,η2aw2Lδℓ4}=cℓΓlog⁡yq≥Γlog⁡yq\begin{aligned} R(E\cap[y_q,2y_q)) &\ge\frac c{\log y_q} \max\left\{\frac\eta{L^\delta\ell^2}, \frac{\eta^2a}{w^2L^\delta\ell^4}\right\}\\ &=\frac{c\ell\Gamma}{\log y_q} \ge\frac\Gamma{\log y_q} \end{aligned}

for large NN. The spare factor ℓ\ell absorbs fixed constants. The selected bin base obeys min⁡E/2≤yq≤max⁡E\min E/2\le y_q\le\max E, so in particular yq≤N/(qdq)y_q\le N/(qd_q). Its reciprocal mass is at most a fixed constant; hence log⁡yq≫Γ≫L3ε\log y_q\gg\Gamma\gg L^{3\varepsilon}.

Now fix q1,q2∈Dhq_1,q_2\in\mathcal D_h, set y=min⁡(yq1,yq2)y=\min(y_{q_1},y_{q_2}), and define the following set of primes:

P={p:exp⁡((log⁡N)ε)≤p≤exp⁡((log⁡y)(log⁡N)−ε)}.\mathcal P=\{p:\exp((\log N)^\varepsilon)\le p \le\exp((\log y)(\log N)^{-\varepsilon})\}.

The preceding lower bound on log⁡y\log y makes this interval nonempty. Its upper prime logarithm is at most (log⁡yq)L−ε(\log y_q)L^{-\varepsilon} for either bin. As L−ε≤1/log⁡log⁡yqL^{-\varepsilon}\le1/\sqrt{\log\log y_q} eventually, Lemma 2.4 applies to both bins. For q=q1,q2q=q_1,q_2, let

Pq={p∈P:p∤m for every m∈T~q∩[yq,2yq)}.\mathcal P_q=\{p\in\mathcal P:p\nmid m \text{ for every }m\in\widetilde T_q\cap[y_q,2y_q)\}.

Applying Lemma 2.4 to [yq,2yq)[y_q,2y_q), all selected integers avoid the primes in Pq\mathcal P_q, giving

R(Pq)≤−log⁡ ⁣(ΓCslog⁡yq).R(\mathcal P_q)\le-\log\!\left(\frac\Gamma{C_s\log y_q}\right).

Here CsC_s is an absolute sieve comparison constant, independent of the statement constant CC. The sieve gives an upper bound proportional to ∏p∈Pq(1−1/p)\prod_{p\in\mathcal P_q}(1-1/p) for the reciprocal mass, which is at most a constant times exp⁡(−R(Pq))\exp(-R(\mathcal P_q)). Combining this with the proved lower bound gives the displayed logarithm. By the reciprocal-prime estimate in Theorem 2.1,

R(P∖(Pq1∪Pq2))≥R(P)−R(Pq1)−R(Pq2)≥log⁡log⁡y2(log⁡N)2ε+log⁡ΓCslog⁡yq1+log⁡ΓCslog⁡yq2=log⁡Γ22Cs2(log⁡N)2εlog⁡max⁡(yq1,yq2)≥log⁡Γ22Cs2(log⁡N)2ε(log⁡(N/M)+(log⁡N)1−δ)≥1.\begin{aligned} R(\mathcal P\setminus(\mathcal P_{q_1}\cup\mathcal P_{q_2})) &\ge R(\mathcal P)-R(\mathcal P_{q_1})-R(\mathcal P_{q_2})\\ &\ge\log\frac{\log y}{2(\log N)^{2\varepsilon}} +\log\frac\Gamma{C_s\log y_{q_1}} +\log\frac\Gamma{C_s\log y_{q_2}}\\ &=\log\frac{\Gamma^2} {2C_s^2(\log N)^{2\varepsilon}\log\max(y_{q_1},y_{q_2})}\\ &\ge\log\frac{\Gamma^2} {2C_s^2(\log N)^{2\varepsilon}(\log(N/M)+(\log N)^{1-\delta})} \ge1. \end{aligned}

The penultimate inequality uses yq≤N/(qdq)y_q\le N/(qd_q) and the lower bound on qdqqd_q. The final inequality uses the proposition's last hypothesis, choosing its absolute constant C≥2eCs2C\ge2eC_s^2.

For p∈P∖Pqp\in\mathcal P\setminus\mathcal P_q, some n∈Tq∗n\in T_q^* has p∣n/(qdq)p\mid n/(qd_q). Since ∣hn∣<K/2|h_n|<K/2, the integer h−hn∈Ihh-h_n\in I_h is a multiple of nn, hence a multiple of pqdqpqd_q. Uniqueness of the multiple of qdqqd_q in IhI_h gives h−hn=xqh-h_n=x_q, and therefore p∣xqp\mid x_q. Every prime in P∖(Pq1∪Pq2)\mathcal P\setminus(\mathcal P_{q_1}\cup\mathcal P_{q_2}) divides xq1−xq2x_{q_1}-x_{q_2}. Their reciprocal sum is at least 1 and each is at least u=exp⁡((log⁡N)ε)u=\exp((\log N)^\varepsilon), so there are at least uu such primes and their product is at least uu>Nu^u>N. But ∣xq1−xq2∣<K≤N|x_{q_1}-x_{q_2}|<K\le N. Thus xq1=xq2x_{q_1}=x_{q_2}. There is a single integer z∈Ihz\in I_h divisible by every element of Dh\mathcal D_h, and hence by [Dh][\mathcal D_h]. The source calls this integer xx, overloading the target numerator; zz separates those roles here.

Summing the minor arcs

Fix D⊆QAD\subseteq\mathcal Q_A. If Dh=D\mathcal D_h=D, a multiple of [D][D] lies in IhI_h. Among a complete period of QQ values of hh, the number of such hh is bounded by

(K+1)[QA][D]≤N∏q∈QA∖Dq≤N∣QA∖D∣+1.(5.4)(K+1)\frac{[\mathcal Q_A]}{[D]} \le N\prod_{q\in\mathcal Q_A\setminus D}q \le N^{|\mathcal Q_A\setminus D|+1}. \tag{5.4}

For ∣h∣>M/2≥K/2|h|>M/2\ge K/2 in the centered period, Dh≠QA\mathcal D_h\ne\mathcal Q_A: otherwise a multiple of QQ would lie within K/2K/2 of such hh, which is impossible. Combining (5.3) and (5.4), and using at most NsN^s choices of a complement of size ss, yields

1Q∑D⊊QAN∣QA∖D∣+1N−10∣QA∖D∣≤1Q∑s≥1Ns+1NsN−10s≤2QN.\begin{aligned} \frac1Q\sum_{D\subsetneq\mathcal Q_A} N^{|\mathcal Q_A\setminus D|+1}N^{-10|\mathcal Q_A\setminus D|} &\le\frac1Q\sum_{s\ge1}N^{s+1}N^sN^{-10s}\\ &\le\frac2{QN}. \end{aligned}

The major arcs therefore contribute at least 3/(4Q)3/(4Q) and the minor arcs have absolute contribution at most 2/(QN)2/(QN). For large NN, (5.2) is at least 1/(2Q)1/(2Q). Subtracting the concentration bound leaves positive probability that R(B)=x/QR(B)=x/Q, as required.

Source corrections and verification

The source's p. 17 residue definition omits the absolute value, and TqT_q is printed as a cardinality rather than a set. The proof above uses the meanings required by the ensuing argument. Its Fourier threshold retains (1−τ)−1(1-\tau)^{-1}; the existing L3L^3 slack in the bound on SS absorbs that factor. The source's assertion R(A)≥ηR(A)\ge\eta is replaced by the smallest-prime sieve argument that gives the needed major-arc cardinality.

The actual Lemma 5.1 scale has mass parameter η/2\eta/2 and denominator ℓ3\ell^3. The printed pp. 17–18 instead mix powers ℓ2\ell^2 and ℓ\ell; the proof keeps the actual H∗H_* and includes the initial dyadic bin. Weighted pigeonholing retains the claimed Γ\Gamma, with a spare factor ℓ\ell to absorb constants. The feasibility estimates explicitly give δ<1/2\delta<1/2, H∗→∞H_*\to\infty, and Γ≫L3ε\Gamma\gg L^{3\varepsilon}, closing its invocation and prime-interval checks. These bounded corrections received independent review before incorporation (the source checks and preliminary review). The exact rewritten proof also passed independent blind review on 2026-09-18, retained as the fresh main-proof review with its distinct grade; the earlier main-proof review was ruled on 2026-09-18 a coordinated compilation check, not an independent review. No assertion is made about changes in the uninspected published version.

Dependencies

  • Theorem 2.1: bounds the common denominator and the reciprocal mass of the prime interval.
  • Lemma 2.4: bounds the exceptional primes avoided by the selected dyadic set.
  • Fact 2.5: the modulus estimate for each Fourier factor.
  • Lemma 2.6: concentration around the target reciprocal sum.
  • Lemma 3.1: positive contribution from major arcs.
  • Lemma 5.1: selects a divisor with reciprocal mass and a lower bound on scaled elements in its proved application form.

The source credits Croot [7] and Bloom [4, Propositions 2 and 3] for the proof framework. The elementary Fourier orthogonality argument is included above and is not an additional black-box dependency on Proposition 3.2.

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