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Collision Counts for the Sum of Proper Divisors

../

evidence/: Exact census of collisions s(n) = s(n') through 10^10 in classes cut out by s(n)/n, by the number of prime factors and by the largest prime factor, with an independent small-range reference and external count checks.

large_prime_class_average: Exact local factors and a Brun–Titchmarsh compatibility argument bound the averaged sieve input G1 of the large-prime class, after removing few inputs, except for common divisors of s(a) and s(a') that divide a'-a and exceed every prime factor of both cofactors by a fixed power; that core is open.

rough_prime_local_density: For at least three free primes on each side, the collision polynomial has uniformly summable local factors away from its coefficients. After a negligible removal of small cofactors, their full local majorants have the required reciprocal-weighted average. The count of prime solutions in integer boxes remains unproved.

uniform_two_form_sieve: An elementary Selberg-weight construction proves the uniform sieve input G0 for the large-prime class, including nonprimitive forms, the interval enlargement and a remainder absorbed uniformly in the main term.


This lead's results that are not drawn from a cited source are Plasma AI's, credited to Plasma AI.

Current review

The independent review of 2026-10-16, accepted by a separate grade, found Theorems A and B and every specified analytic mathematical consequence through the semiprime separation inequality refutation-failed. This records the grader's tier-1 judgment for those exact propositions at the source interfaces retained in the verification record. It establishes neither (D) nor a solution of Problem 955. The numerical census, the G0/G1/G2 route and the rough-prime classes are outside that examination and retain author standing.

The frozen subject contains an unsupported assertion about what is known concerning equivalence of (D). Affirmative certification of that assertion is void; no disproof is given. The current D paragraph makes only the grade-authorized body correction to "The argument does not establish the converse." Other examined mathematical statements and proofs are unchanged, apart from standing descriptions. The later excerpt is separately identified and was not the reviewer's subject.

The reviewer received excluded motivational advocacy, which the separate grader ruled immaterial to this examination under the content test. The exposure and ruling remain disclosed. The external PNT, Mertens and PPT premises were checked at their supplied statement interfaces; original source proofs and PDF fidelity are not certified.

Target and conventions

The target is Problem 955, whose page records the general assertion as open: for s(n)=σ(n)−ns(n)=\sigma(n)-n, does every set A⊆NA\subseteq\mathbb N of natural density zero have a preimage s−1(A)s^{-1}(A) of natural density zero? Nothing on this page changes that status. Here inputs are positive integers, and s(1)=0s(1)=0.

For x≥1x\ge1 and m≥0m\ge0 write rx(m)=#{n≤x:s(n)=m}r_x(m)=\#\{n\le x:s(n)=m\}. For a set SS of admitted inputs, which may depend on xx, write rS,x(m)r_{S,x}(m) for the number of n∈S∩[1,x]n\in S\cap[1,x] with s(n)=ms(n)=m, RS(x)=#(S∩[1,x])R_S(x)=\#(S\cap[1,x]), and

CS(x)=∑mrS,x(m)2=#{(n,n′)∈(S∩[1,x])2: s(n)=s(n′)}.C_S(x)=\sum_m r_{S,x}(m)^2 =\#\{(n,n')\in(S\cap[1,x])^2:\ s(n)=s(n')\}.

Pairs are ordered and the diagonal n=n′n=n' is included. So CS(x)−RS(x)C_S(x)-R_S(x) counts the ordered pairs of distinct inputs with equal values, and (CS(x)−RS(x))/2(C_S(x)-R_S(x))/2 the unordered ones.

The route recorded here is the second-moment route: if few pairs collide, Cauchy–Schwarz bounds the number of inputs that any sparse target can capture. The sections below show which form of that route is false, which form is exactly as strong as the problem, and what an exact computation shows about each.

The density-zero form is false

The proposed form removes a density-zero set of degenerate inputs, such as the semiprimes with s(pq)=p+q+1s(pq)=p+q+1 for distinct primes p,qp,q, and asks for CS(x)=O(x)C_S(x)=O(x) for the rest. No density-zero exclusion can give this.

Theorem A. Let Ex⊆[1,x]E_x\subseteq[1,x] satisfy ∣Ex∣=o(x)|E_x|=o(x) and put Sx=[1,x]∖ExS_x=[1,x]\setminus E_x. Then CSx(x)/x→∞C_{S_x}(x)/x\to\infty.

Proof. Fix δ∈(0,1/10]\delta\in(0,1/10] and put z=1/δz=1/\delta and Z=100zZ=100z. Let RZ\mathcal R_Z be the set of positive integers with no prime factor at most ZZ (so 1∈RZ1\in\mathcal R_Z), let mZ=∏q≤Z(1−1/q)m_Z=\prod_{q\le Z}(1-1/q), and let f(k)=∑q∣k1/(q−1)f(k)=\sum_{q\mid k}1/(q-1), summed over the primes qq dividing kk.

A class with small s(n)/ns(n)/n. Let VδV_\delta be the set of n=pkn=pk with pp prime, z/1.8<p≤z/1.1z/1.8<p\le z/1.1, k∈RZk\in\mathcal R_Z and f(k)≤δ/10f(k)\le\delta/10. Since p<Zp<Z, p∤kp\nmid k, so σ(n)/n=(1+1/p) σ(k)/k\sigma(n)/n=(1+1/p)\,\sigma(k)/k and

1≤σ(k)k≤∏q∣k(1−1q)−1≤ef(k)≤1+0.11 δ,1\le\frac{\sigma(k)}{k}\le\prod_{q\mid k}\Bigl(1-\frac1q\Bigr)^{-1} \le e^{f(k)}\le1+0.11\,\delta,

so δ≤1/p≤s(n)/n≤(1+1.8δ)(1+0.11δ)−1≤2δ\delta\le1/p\le s(n)/n\le(1+1.8\delta)(1+0.11\delta)-1\le2\delta. The pair (p,k)(p,k) is determined by nn, since pp is the only prime factor of nn at most ZZ.

Its size. RZ\mathcal R_Z is a union of residue classes modulo ∏q≤Zq\prod_{q\le Z}q, so #(RZ∩[1,y])=mZy+OZ(1)\#(\mathcal R_Z\cap[1,y])=m_Zy+O_Z(1). For a prime q>Zq>Z, the members of RZ\mathcal R_Z divisible by qq are exactly the qk′qk' with k′∈RZk'\in\mathcal R_Z. Hence

∑k≤yk∈RZf(k)=∑Z<q≤y#(RZ∩[1,y/q])q−1≤mZy∑m>Z1m(m−1)+OZ(log⁡log⁡y)≤1.01 mZyZ+OZ(log⁡log⁡y),\sum_{\substack{k\le y\\ k\in\mathcal R_Z}}f(k) =\sum_{Z<q\le y}\frac{\#(\mathcal R_Z\cap[1,y/q])}{q-1} \le m_Zy\sum_{m>Z}\frac1{m(m-1)}+O_Z(\log\log y) \le\frac{1.01\,m_Zy}{Z}+O_Z(\log\log y),

using ∑m>Z1/(m(m−1))=1/⌊Z⌋\sum_{m>Z}1/(m(m-1))=1/\lfloor Z\rfloor and Z≥1000Z\ge1000. By Markov's inequality at most (10/δ) 1.01 mZy/Z+o(y)≤0.11 mZy+o(y)(10/\delta)\,1.01\,m_Zy/Z+o(y)\le0.11\,m_Zy+o(y) members of RZ∩[1,y]\mathcal R_Z\cap[1,y] have f(k)>δ/10f(k)>\delta/10. Summing over the finitely many pp,

#(Vδ∩[1,x])≥(dδ−o(1)) x,dδ=0.89 mZ∑z/1.8<p≤z/1.11p.\#(V_\delta\cap[1,x])\ge(d_\delta-o(1))\,x,\qquad d_\delta=0.89\,m_Z\sum_{z/1.8<p\le z/1.1}\frac1p.

As δ→0\delta\to0, Mertens' product theorem gives mZ∼e−γ/log⁡(1/δ)m_Z\sim e^{-\gamma}/\log(1/\delta) and the prime number theorem gives ∑z/1.8<p≤z/1.11/p∼log⁡(18/11)/log⁡(1/δ)\sum_{z/1.8<p\le z/1.1}1/p\sim\log(18/11)/\log(1/\delta). Since 0.89 e−γlog⁡(18/11)>0.240.89\,e^{-\gamma}\log(18/11)>0.24, every sufficiently small δ\delta has dδ≥0.2/log⁡2(1/δ)d_\delta\ge0.2/\log^2(1/\delta). The convergence is slow, because log⁡Z=log⁡(1/δ)+log⁡100\log Z=\log(1/\delta)+\log100; the bound is asymptotic and is not claimed for every δ≤1/10\delta\le1/10.

Pigeonhole. The set Nx=(Vδ∩[1,x])∖ExN_x=(V_\delta\cap[1,x])\setminus E_x has at least (dδ−o(1))x(d_\delta-o(1))x members, and their values s(n)s(n) lie in [1,2δx][1,2\delta x]. By Cauchy–Schwarz over those values,

CSx(x)≥∑m≤2δxrNx,x(m)2≥∣Nx∣22δx≥(dδ−o(1))22δ x.C_{S_x}(x)\ge\sum_{m\le2\delta x}r_{N_x,x}(m)^2\ge\frac{|N_x|^2}{2\delta x} \ge\frac{(d_\delta-o(1))^2}{2\delta}\,x .

So $\liminf_x C_{S_x}(x)/x\ge d_\delta^2/(2\delta)\ge 0.02/(\delta\log^4(1/\delta))$ for every small δ\delta, which is unbounded as δ→0\delta\to0. □\square

The mechanism is general: the inputs of VδV_\delta, whose least prime factor is near 1/δ1/\delta and whose other prime factors are large, have their values in [1,2δx][1,2\delta x] although they range over [1,x][1,x], and they form a proportion of order 1/log⁡2(1/δ)1/\log^2(1/\delta) of all inputs. The degenerate families that an exclusion is meant to remove, such as the semiprimes, are only the extreme case. The same argument with ∣Ex∣≤εx|E_x|\le\varepsilon x gives

lim inf⁡x→∞CSx(x)x≥sup⁡δ: dδ>ε(dδ−ε)22δ,\liminf_{x\to\infty}\frac{C_{S_x}(x)}{x} \ge\sup_{\delta:\ d_\delta>\varepsilon}\frac{(d_\delta-\varepsilon)^2}{2\delta},

and taking δ=exp⁡(−0.1/ε)\delta=\exp(-\sqrt{0.1/\varepsilon}), where dδ≥2εd_\delta\ge2\varepsilon for small ε\varepsilon, shows that the right side is at least (ε2/2)exp⁡(0.1/ε)(\varepsilon^2/2)\exp(\sqrt{0.1/\varepsilon}). Any constant KK in the corrected form below must therefore grow faster than every power of 1/ε1/\varepsilon.

This proof has the independent review and grade described above. Its external inputs are the prime number theorem and Mertens' product theorem, at the retained statement-interface reading depth.

An equivalent form of the problem

The second-moment route loses nothing in principle once the exceptional set may have small positive density and the constant may depend on it.

Theorem B. The following are equivalent.

  1. Every A⊆NA\subseteq\mathbb N of natural density zero has s−1(A)s^{-1}(A) of natural density zero.
  2. The fiber sizes are tight: lim⁡T→∞lim sup⁡x→∞x−1#{n≤x:rx(s(n))>T}=0\lim_{T\to\infty}\limsup_{x\to\infty}x^{-1}\#\{n\le x:r_x(s(n))>T\}=0.
  3. For every ε>0\varepsilon>0 there are KK and x0x_0 such that every x≥x0x\ge x_0 has a set Ex⊆[1,x]E_x\subseteq[1,x] with ∣Ex∣≤εx|E_x|\le\varepsilon x and C[1,x]∖Ex(x)≤KxC_{[1,x]\setminus E_x}(x)\le Kx.
  4. For every ε>0\varepsilon>0 there are η>0\eta>0 and x0x_0 such that #{n≤x:s(n)∈B}≤εx\#\{n\le x:s(n)\in B\}\le\varepsilon x for every x≥x0x\ge x_0 and every set B⊆N∪{0}B\subseteq\mathbb N\cup\{0\} of at most ηx\eta x integers.

Proof. (2 ⇒ 3) Given ε\varepsilon, choose TT and x0x_0 with #{n≤x:rx(s(n))>T}≤εx\#\{n\le x:r_x(s(n))>T\}\le\varepsilon x for x≥x0x\ge x_0, and let ExE_x be that set. Every value taken on [1,x]∖Ex[1,x]\setminus E_x is taken at most TT times there, so C[1,x]∖Ex(x)≤T R[1,x]∖Ex(x)≤TxC_{[1,x]\setminus E_x}(x)\le T\,R_{[1,x]\setminus E_x}(x)\le Tx.

(3 ⇒ 1) Let AA have density zero, and fix ε>0\varepsilon>0 and L≥1L\ge1. For x≥x0x\ge x_0 the inputs n≤xn\le x with s(n)∈As(n)\in A are of three kinds. At most εx\varepsilon x lie in ExE_x. Those with s(n)>Lxs(n)>Lx have σ(n)/n>L+1\sigma(n)/n>L+1, and

∑n≤xσ(n)n=∑d≤x1d⌊xd⌋≤ζ(2) x\sum_{n\le x}\frac{\sigma(n)}n=\sum_{d\le x}\frac1d\Bigl\lfloor\frac xd \Bigr\rfloor\le\zeta(2)\,x

bounds their number by 2x/L2x/L. The rest have values in A∩[0,Lx]A\cap[0,Lx], and Cauchy–Schwarz bounds them by (∣A∩[0,Lx]∣⋅Kx)1/2=o(x)(|A\cap[0,Lx]|\cdot Kx)^{1/2}=o(x). So the upper density of s−1(A)s^{-1}(A) is at most ε+2/L\varepsilon+2/L for all ε\varepsilon and LL.

(1 ⇒ 2) Suppose (2) fails. The quantity in (2) is nonincreasing in TT, so there is η>0\eta>0 such that for every TT arbitrarily large xx have #{n≤x:rx(s(n))>T}>ηx\#\{n\le x:r_x(s(n))>T\}>\eta x. Write mw=∏p≤w(1−1/p)m_w=\prod_{p\le w}(1-1/p) and fix L≥4L\ge4 with L−1/2+mL≤η/4L^{-1/2}+m_{\sqrt L}\le\eta/4. An input n∈(x/L,x]n\in(x/\sqrt L,x] with s(n)<x/Ls(n)<x/L has σ(n)/n<1+L−1/2\sigma(n)/n<1+L^{-1/2}, hence no prime factor at most L\sqrt L; so #{n≤x:s(n)<x/L}≤(η/4)x+OL(1)\#\{n\le x:s(n)<x/L\}\le(\eta/4)x+O_L(1). Put x0=1x_0=1 and choose inductively xkx_k with #{n≤xk:rxk(s(n))>k}>ηxk\#\{n\le x_k:r_{x_k}(s(n))>k\}>\eta x_k, xk≥k2L xk−1x_k\ge k^2L\,x_{k-1} and OL(1)≤ηxk/4O_L(1)\le\eta x_k/4, and let

Ak={m≥xk/L: rxk(m)>k},A=⋃kAk.A_k=\{m\ge x_k/L:\ r_{x_k}(m)>k\},\qquad A=\bigcup_kA_k .

Then #{n≤xk:s(n)∈A}≥ηxk−(η/2)xk\#\{n\le x_k:s(n)\in A\}\ge\eta x_k-(\eta/2)x_k, so s−1(A)s^{-1}(A) has upper density at least η/2\eta/2. On the other hand ∣Ak∣<xk/k|A_k|<x_k/k, because ∑mrxk(m)≤xk\sum_mr_{x_k}(m)\le x_k, so ∑j<k∣Aj∣<∑j<kxj≤k xk−1\sum_{j<k}|A_j|<\sum_{j<k}x_j\le k\,x_{k-1}. If kk is the largest index with xk/L≤yx_k/L\le y, then A∩[1,y]⊆A1∪⋯∪AkA\cap[1,y]\subseteq A_1\cup\dots\cup A_k and

∣A∩[1,y]∣y≤Lxk(xkk+k xk−1)≤Lk+1k,\frac{|A\cap[1,y]|}{y}\le\frac{L}{x_k}\Bigl(\frac{x_k}{k}+k\,x_{k-1}\Bigr) \le\frac{L}{k}+\frac1k ,

so AA has density zero and (1) fails.

(2 ⇔ 4) If (2) holds, choose TT with $#{n\le x:r_x(s(n))>T}\le\varepsilon x/2$ for large xx and put η=ε/(2T)\eta=\varepsilon/(2T): a set BB of at most ηx\eta x values captures at most εx/2\varepsilon x/2 inputs in fibers larger than TT and at most TηxT\eta x others. If (4) holds, take T=1/ηT=1/\eta; the set B={m:rx(m)>T}B=\{m:r_x(m)>T\} has fewer than x/T=ηxx/T=\eta x members, so it captures at most εx\varepsilon x inputs. The quantity in (2) is therefore at most ε\varepsilon for every T≥1/ηT\ge1/\eta, and ε\varepsilon is arbitrary. □\square

This proof has the independent review and grade described above. Statement 4 places the problem beside [[../library/arithmetic_functions/pollack_2018_divisor_sum_fibers/theorem_1_2|Pollack, Pomerance and Thompson's Theorem 1.2, which proves the same uniform control for targets of total size at most x1/2+ϵ(x)x^{1/2+\epsilon(x)}]]: the problem asks for it at size ηx\eta x, with ε→0\varepsilon\to0 as η→0\eta\to0. The problem page's countermodel shows that control at the smaller size cannot be extended by an abstract argument; Theorem B says that control at linear size is exactly what is needed.

Statement 3 is the corrected form of the route. Its natural explicit version uses the sets

D(δ)={n composite: s(n)≥δn}.D(\delta)=\{n\ \text{composite}:\ s(n)\ge\delta n\}.

An input outside D(δ)D(\delta) is 11, a prime, or has no prime factor at most 1/δ1/\delta, so the complement of D(δ)D(\delta) has upper density at most ∏p≤1/δ(1−1/p)→0\prod_{p\le1/\delta}(1-1/p)\to0. The bound

(D)CD(δ)(x)≤Kδ xfor every fixed δ>0 and all large x\text{(D)}\qquad C_{D(\delta)}(x)\le K_\delta\,x\quad\text{for every fixed }\delta>0\text{ and all large }x

therefore implies statement 3, by choosing δ\delta with ∏p≤1/δ(1−1/p)<ε\prod_{p\le1/\delta}(1-1/p)<\varepsilon and Ex=[1,x]∖D(δ)E_x=[1,x]\setminus D(\delta), and hence the problem. The argument does not establish the converse. The class VδV_\delta of Theorem A, apart from its finitely many primes, lies in D(δ)D(\delta), so the pigeonhole step gives Kδ≥0.02/(δlog⁡4(1/δ))K_\delta\ge0.02/(\delta\log^4(1/\delta)) for small δ\delta, and Kδ→∞K_\delta\to\infty. The semiprimes in D(δ)D(\delta) are harmless. For distinct primes p<qp<q, s(pq)=p+q+1≥δpqs(pq)=p+q+1\ge\delta pq forces p≤3/δp\le3/\delta, and s(p2)=p+1s(p^2)=p+1 comes from one prime square at most; so each value is taken by at most π(3/δ)+1\pi(3/\delta)+1 semiprimes in D(δ)D(\delta), and they contribute at most (π(3/δ)+1)x(\pi(3/\delta)+1)x to the sum of squares, which (r1+r2)2≤2r12+2r22(r_1+r_2)^2\le2r_1^2+2r_2^2 separates from the rest.

Exact census through 10^10

The census computes RR and CC exactly for composite inputs n≤xn\le x in the classes

Dk={n composite: 2ks(n)≥n},DTk={n∈Dk: Ω(n)≥3},D_k=\{n\ \text{composite}:\ 2^ks(n)\ge n\},\qquad DT_k=\{n\in D_k:\ \Omega(n)\ge3\},

for k=0,…,14k=0,\dots,14, and for all composites, written QQ, and the composites with Ω(n)≥3\Omega(n)\ge3, written TT; Ω\Omega counts prime factors with multiplicity. So Dk=D(2−k)D_k=D(2^{-k}), D0D_0 is the set of abundant and perfect composites, and TT is the proposed density-zero exclusion: it removes 11, the primes and every input with exactly two prime factors, including the prime squares with s(p2)=p+1s(p^2)=p+1. By Landau's estimate at most O(xlog⁡log⁡x/log⁡x)O(x\log\log x/\log x) inputs n≤xn\le x are removed, so the excluded set has density zero, as the proposed route requires. The checkpoints are x=⌊103+j/4⌋x=\lfloor10^{3+j/4}\rfloor, j=0,…,28j=0,\dots,28, so the range reaches 101010^{10}. All arithmetic is exact. The program and its checks are described in the evidence record.

The ratio C/xC/x at each decade, rounded to four decimals:

xxQQTTD0D_0D2D_2D4D_4D6D_6DT2DT_2DT4DT_4DT6DT_6
10510^53.23151.38790.38021.45141.93322.49301.19481.37901.3879
10610^64.30501.62200.39441.51322.02652.50001.29781.55571.6220
10710^76.01381.85040.40421.55332.06982.63201.36861.66661.8450
10810^89.03912.07980.40981.57582.09492.68331.41421.74271.9890
10910^914.87692.32320.41281.58932.11012.69861.44581.79772.0846
101010^{10}26.84232.59490.41431.59682.11862.71211.46761.83772.1603

At x=109x=10^9 the exact restricted values are CT=2323154413C_T=2323154413 and RT=788363929R_T=788363929, with 211636071211636071 excluded inputs. At x=1010x=10^{10} the exact values are CT=25949106637C_T=25949106637 with RT=8051171045R_T=8051171045, CD0=4143350299C_{D_0}=4143350299 with RD0=2476238927R_{D_0}=2476238927, and CD4=21185514129C_{D_4}=21185514129 with RD4=8188172635R_{D_4}=8188172635. The proportions of n≤1010n\le10^{10} outside each class are 0.19490.1949 for TT, 0.75240.7524 for D0D_0, 0.29970.2997 for D2D_2, 0.18120.1812 for D4D_4 and 0.12800.1280 for D6D_6.

Reading. No numerical tolerance for leveling off was fixed in advance. This page reads "levels off" as decade increments of C/xC/x that shrink from one decade to the next, and "does not level off" as increments that do not shrink. The reading was chosen when the computation was made, so the census is exploratory evidence, not a test of a prediction stated in advance.

  • The ratio for QQ rises by a factor of about 1.81.8 from 10910^9 to 101010^{10}. Balanced semiprimes alone force superlinear collisions: there are ≫x/log⁡2x\gg x/\log^2x distinct products pqpq with x/2<p<q≤x\sqrt x/2<p<q\le\sqrt x, and their values p+q+1p+q+1 occupy O(x)O(\sqrt x) integers. Cauchy–Schwarz therefore gives CQ(x)≫x3/2/log⁡4xC_Q(x)\gg x^{3/2}/\log^4x. This aggregate argument uses the prime number theorem; it asserts no estimate for any individual Goldbach sum.
  • TT does not level off. Its decade increments from 10610^6 to 101010^{10} are 0.2280.228, 0.2290.229, 0.2430.243 and 0.2720.272. Theorem A predicts unbounded growth for every density-zero exclusion, but its pigeonhole bound is far below this observed rate at these scales; the observed rate is not derived here. The growth sits in inputs with small s(n)/ns(n)/n. At 10610^6 the classes TT and DT6DT_6 differ by seven inputs, the prime cubes p3p^3 with 64<p<10064<p<100, and their ratios agree to four decimals; at 101010^{10} the ratios differ by 0.4350.435, and DT6DT_6 alone decelerates.
  • Every DkD_k with k≤7k\le7 and every DTkDT_k with k≤6k\le6 levels off over the last three decades. From 10610^6 to 101010^{10} the increments of D0D_0 are 0.00980.0098, 0.00550.0055, 0.00300.0030, 0.00150.0015; of D4D_4 0.04340.0434, 0.02510.0251, 0.01520.0152, 0.00850.0085; of DT2DT_2 0.07080.0708, 0.04570.0457, 0.03150.0315, 0.02190.0219; of DT6DT_6 0.22300.2230, 0.14400.1440, 0.09560.0956, 0.07570.0757. Classes with larger kk are still in transition: the restriction s(n)≥2−kns(n)\ge2^{-k}n removes nothing when x≤4kx\le4^k, since s(n)>ns(n)>\sqrt n for composite nn.
  • Large fibers are rare in the restricted classes. At 101010^{10} the largest value multiplicity is 4747 in D0D_0 and 6868 in D4D_4, against 124124 in TT; the number of admitted inputs lying in fibers of more than eight inputs, divided by xx rather than by RS(x)R_S(x), is 0.00070.0007 in D0D_0, 0.01280.0128 in D4D_4 and 0.04720.0472 in TT.

Split by the largest prime factor. A second run of the census flags the inputs whose largest prime factor exceeds n\sqrt n, a set of density log⁡2\log2, which is the model of the class S1 of the sketch below; the other composites model S2. The table gives the ordered off-diagonal pairs per input range, (C−R)/x(C-R)/x, inside S1, inside S2, and across the two (both orders), within DkD_k:

xxS1, k=0k=0S2, k=0k=0across, k=0k=0S1, k=2k=2S2, k=2k=2across, k=2k=2S1, k=4k=4S2, k=4k=4across, k=4k=4
10610^60.05120.02270.07300.42870.06180.32260.61710.09670.4930
10710^70.06010.02250.07400.45800.06570.32910.66790.09310.4898
10810^80.06670.02180.07370.47690.06780.33080.69050.09560.4900
10910^90.07150.02100.07270.48790.06910.33200.70020.09890.4922

For k≤4k\le4 the S1 and cross components level off, the S2 components for k≤2k\le2 level off or decrease, and the S2 component for k=4k=4 stays between 0.0930.093 and 0.0990.099. The collisions inside S2 are far fewer than inside S1. Without the restriction the S2 part does not level off: over all composites with no prime factor above n\sqrt n, (C−R)/x(C-R)/x is 0.12670.1267, 0.16670.1667, 0.21580.2158 and 0.27790.2779 at 106,…,10910^6,\dots,10^9, with growing increments, again from inputs with small s(n)/ns(n)/n.

The census cannot prove any asymptotic statement, and over these few decades it cannot separate convergence of C/xC/x from growth like log⁡log⁡x\log\log x. It does show that the proposed density-zero route fails its own test already at these scales, and that nothing in the corrected classes, or in their split by the largest prime factor, contradicts (D).

Proof sketch of the corrected route

Target. Statement 3 of Theorem B, through the sufficient bound (D) or another family of exceptional sets whose upper densities tend to zero. Theorems A and B have the independent review described above. The argument in this section remains conditional on G1, whose trimmed form is reduced to Gap G1-core below, and on G2. Its coefficient-uniform sieve input G0 has a complete author-recorded proof.

Splitting. For a disjoint union of two admitted classes, (r1+r2)2≤2r12+2r22(r_1+r_2)^2\le2r_1^2+2r_2^2, so bounds for collisions inside the classes control collisions between them too. A finite number of classes is allowed, with that number depending on the discarded proportion.

Class S1: a prime factor above x1/2+ηx^{1/2+\eta}. Fix δ>0\delta>0 and 0<η<1/20<\eta<1/2, put y=x1/2−ηy=x^{1/2-\eta}, and let S1(x)S_1(x) consist of the composite n=aP≤xn=aP\le x with PP prime, P>x1/2+ηP>x^{1/2+\eta} and s(n)≥δns(n)\ge\delta n. Then P∤aP\nmid a, 2≤a<y2\le a<y, and

s(aP)=s(a)P+σ(a).s(aP)=s(a)P+\sigma(a).

Since σ(a)/a≤1+log⁡a\sigma(a)/a\le1+\log a, the identity s(aP)/(aP)=s(a)/a+σ(a)/(aP)s(aP)/(aP)=s(a)/a+\sigma(a)/(aP) implies s(a)≥δa/2s(a)\ge\delta a/2 for sufficiently large xx, uniformly over these cofactors. The same cofactor aa gives no off-diagonal collision because s(a)>0s(a)>0.

For a≠a′a\ne a' put g=gcd⁡(s(a),s(a′))g=\gcd(s(a),s(a')) and h=σ(a′)−σ(a)h=\sigma(a')-\sigma(a). A collision requires

s(a)P−s(a′)P′=h,g∣h.s(a)P-s(a')P'=h,\qquad g\mid h.

If h=0h=0, there is no collision in these ranges: both large primes exceed s(a)s(a) and s(a′)s(a') for large xx, so s(a)P=s(a′)P′s(a)P=s(a')P' forces P=P′P=P' and s(a)=s(a′)s(a)=s(a'); together with h=0h=0 this forces a=a′a=a'. For h≠0h\ne0 and g∣hg\mid h, write the integer solutions as

P=u+βt,P′=v+λt,β=s(a′)/g,λ=s(a)/g.P=u+\beta t,\quad P'=v+\lambda t,\qquad \beta=s(a')/g,\quad\lambda=s(a)/g.

The admissible parameters lie in an interval contained in one of length L=xg/(a s(a′))L=xg/(a\,s(a')). This is an upper length supplied by the first prime's range, not a lower bound on the actual intersection of the two prime ranges. It satisfies L≥x2η/(1+log⁡x)L\ge x^{2\eta}/(1+\log x), so it is possible to enlarge the interval to this length when seeking an upper bound.

For these pairs let ωa,a′(p)\omega_{a,a'}(p) be the number of residues tt modulo pp where at least one of the two forms vanishes, and define

Sz(a,a′)=∏p≤z(1−ωa,a′(p)p)(1−1p)−2.\mathfrak S_z(a,a')=\prod_{p\le z} \Bigl(1-\frac{\omega_{a,a'}(p)}p\Bigr)\Bigl(1-\frac1p\Bigr)^{-2}.

A different integer solution (u,v)(u,v) translates tt and leaves this quantity unchanged. Pairs with no solution, and pairs with h=0h=0, are omitted from the sum below; no singular series is needed for them.

Uniform sieve input G0. For every eligible pair,

N(a,a′)≪ηxga s(a′)log⁡2x Sx(a,a′).N(a,a')\ll_\eta \frac{xg}{a\,s(a')\log^2x}\,\mathfrak S_x(a,a').

The coefficient-uniform two-form argument proves this by an explicit Selberg-weight construction. Its interval error is bounded by z2(1+log⁡z)10z^2(1+\log z)^{10}, uniformly in all coefficients. With z=L1/4z=L^{1/4} and L≥x2η/(1+log⁡x)L\ge x^{2\eta}/(1+\log x), this error is absorbed in the main term, whose singular series has an absolute positive lower bound whenever the forms are admissible. Nonprimitive forms and the obstruction ω(2)=2\omega(2)=2 give no prime pair in the stated range. The proof also justifies the interval enlargement and the comparison of singular-series cutoffs. G0 therefore needs no separate error sum and no unexamined sieve theorem. It is author-recorded and outside the analytic review.

Set Aδ(y)={2≤a≤y:s(a)≥δa/2}\mathcal A_\delta(y)=\{2\le a\le y:s(a)\ge\delta a/2\} and

Λδ(y;z)=∑a,a′∈Aδ(y), a≠a′h≠0, g∣hg Sz(a,a′)aa′.\Lambda_\delta(y;z)= \sum_{\substack{a,a'\in\mathcal A_\delta(y),\ a\ne a'\\ h\ne0,\ g\mid h}} \frac{g\,\mathfrak S_z(a,a')}{aa'}.

Summing G0 gives

CS1(x)≪ηx+xδlog⁡2xΛδ(x1/2−η;x).C_{S_1}(x)\ll_\eta x+ \frac{x}{\delta\log^2x}\Lambda_\delta(x^{1/2-\eta};x).

Gap G1 (averaged singular series). The missing estimate is Λδ(x1/2−η;x)≪δ,ηlog⁡2x\Lambda_\delta(x^{1/2-\eta};x)\ll_{\delta,\eta}\log^2x for every fixed δ,η\delta,\eta. The prime cutoff and the cofactor cutoff are distinct in this statement. For statement 3 of Theorem B a trimmed form suffices: the same bound after removing a set of cofactors a<ya<y with ∑1/a≤ε′log⁡y\sum1/a\le\varepsilon'\log y, whose inputs number at most 2ε′x2\varepsilon'x. The trimmed form is not G1 as stated for every cofactor, and it does not prove (D) for the whole class.

The averaged estimate for the large-prime class reduces the trimmed form to one estimate, at author standing. Its local lemmas are complete. For an eligible pair and a prime pp, with e1=vp(s(a))e_1=v_p(s(a)), e2=vp(s(a′))e_2=v_p(s(a')), e=vp(g)e=v_p(g) and f=vp(h)f=v_p(h), the factor of g Sx(a,a′)g\,\mathfrak S_x(a,a') is pep/(p−1)p^ep/(p-1) when e1≠e2e_1\ne e_2 or f>ef>e, and pe(1−(p−1)−2)p^e(1-(p-1)^{-2}) otherwise; a pair with e1≠e2e_1\ne e_2 and f>ef>e has no prime solutions. If vp(σ(a))>vp(a)v_p(\sigma(a))>v_p(a) and the same holds for a′a', the factor is exactly pvp(a)p/(p−1)p^{v_p(a)}p/(p-1), and the pair is excluded unless vp(a)=vp(a′)v_p(a)=v_p(a'). Under independent geometric valuation frequencies Pr⁡(vp(a)=e)=(1−1/p)p−e\Pr(v_p(a)=e)=(1-1/p)p^{-e} this factor has mean

∑e≥0(1−1/p)2p−2e pepp−1=1,\sum_{e\ge0}(1-1/p)^2p^{-2e}\,p^e\frac p{p-1}=1,

which is why the small primes balance. The page then restricts to good cofactors: their two largest primes exceed yνy^\nu, (a,σ(a))(a,\sigma(a)) has no prime factor above W=log⁡log⁡y/(4log⁡log⁡log⁡y)W=\log\log y/(4\log\log\log y), and σ\sigma satisfies the small-prime condition above at the cofactor a/P(a)a/P(a); the others carry reciprocal weight O(νlog⁡(1/ν)log⁡y)O(\nu\log(1/\nu)\log y). For good cofactors, every divisor dd of the part of gg above WW fixes the largest prime of aa modulo dd, and the congruence a≡a′(modd)a\equiv a'\pmod d restricts the second largest prime through a quadratic congruence. Removing a further set of reciprocal weight o(log⁡y)o(\log y) ensures that no prime above WW divides both s(a)s(a) and P(a)−P2(a)P(a)-P_2(a). The quadratic roots representing retained cofactors are then simple, giving at most 2ω(d)2^{\omega(d)} classes modulo dd, including all its prime powers. With Brun–Titchmarsh this bounds by O(log⁡2y)O(\log^2y) every part of the trimmed sum except the divisors dd with d≥max⁡(P(a),P(a′))1−κd\ge\max(P(a),P(a'))^{1-\kappa}, for a fixed small κ>0\kappa>0. The density of these good cofactors and the averages of the small-prime and singular-series weights are proved there, with constants not computed explicitly.

Gap G1-core. Bound by O(log⁡2y)O(\log^2y) the part of the trimmed sum coming from common divisors dd of s(a)s(a) and s(a′)s(a') that divide a′−aa'-a and satisfy d1/(1−κ)≥max⁡(P(a),P(a′))d^{1/(1-\kappa)}\ge\max(P(a),P(a')). When such a dd exceeds P(a)P(a), the prime P(a)P(a) is the least positive residue of −σ(c)s(c)−1-\sigma(c)s(c)^{-1} modulo dd, where c=a/P(a)c=a/P(a). The estimate asks that these least residues fall in short initial intervals no more often than their length predicts, on average over the pairs. Counting arguments on the linked page remove further core divisors: those for which a cofactor has its largest prime above d1−κ′′d^{1-\kappa''}, for a small fixed κ′′\kappa''; those for which the two cofactors' largest primes have product at least d1+ϵd^{1+\epsilon}; and those for which one cofactor's two largest primes have product at least d1+ϵd^{1+\epsilon}. The simple-root condition makes these removals valid without a restriction on the radical of dd. What remains are large divisors exceeding, up to the factor dϵd^\epsilon, the product of the two largest of these primes. It is not a local-factor question; it is the same kind of input as the slice estimate G2-bal below.

The reduced coefficients u=s(a)/gu=s(a)/g, v=s(a′)/gv=s(a')/g of an eligible pair satisfy max⁡(u,v)>∏p≤Wp/(1+2/δ)\max(u,v)>\prod_{p\le W}p/(1+2/\delta), by Lemma 7 of the linked page. In particular s(a)=s(a′)s(a)=s(a') gives no retained eligible pair for large yy. A descent must therefore control scaled collisions with unbounded reduced coefficients and the extra congruence, rather than just ordinary cofactor fibers. Removing the largest primes produces affine equations with a generally nonzero right side; no contracting recurrence is derived. Luca and Pomerance avoid this regime only through cofactors m=qℓm=q\ell with ℓ≤x1/10\ell\le x^{1/10}, as recorded on the linked page.

What S1 would give. G0 and G1 imply CS1(x)≪δ,ηxC_{S_1}(x)\ll_{\delta,\eta}x. G0 with the trimmed form of G1 implies the same bound after removing at most εx\varepsilon x inputs, for each ε>0\varepsilon>0. The upper-output truncation in Theorem B then gives #{n∈S1(x):s(n)∈A}=o(x)\#\{n\in S_1(x):s(n)\in A\}=o(x) for every density-zero AA. The number of integers with a prime factor above x1/2+ηx^{1/2+\eta} is (log⁡(2/(1+2η))+o(1))x(\log(2/(1+2\eta))+o(1))x, by summing ⌊x/P⌋\lfloor x/P\rfloor over those primes; the factor is unique. The discarded condition s(n)<δns(n)<\delta n, together with the primes, has upper density tending to zero as δ→0\delta\to0. Therefore G0 and either form of G1 for every δ,η\delta,\eta would bound the upper density of s−1(A)s^{-1}(A) by 1−log⁡21-\log2. This is conditional partial progress, not a conclusion proved by the census or by this sketch.

Class S2: the remaining inputs. Define S2(x)=(D(δ)∩[1,x])∖S1(x)S_2(x)=(D(\delta)\cap[1,x])\setminus S_1(x). The unrestricted complement of the large-prime class has density 1−log⁡(2/(1+2η))1-\log(2/(1+2\eta)), tending to 1−log⁡21-\log2 as η→0\eta\to0; it cannot be discarded as a density-zero family.

The S1 argument supplies no uniform long parameter interval for S2. On input intervals comparable to xx, cofactors can exceed x\sqrt x; for pairs with small gg the upper interval length is then only O(1)O(1) or smaller. This defeats that particular uniform application of the sieve, not every possible use of a large prime factor or another parametrization.

Gap G2. Prove CS2(x)≪δ,ηxC_{S_2}(x)\ll_{\delta,\eta}x, or replace this estimate by another decomposition that proves Theorem B's statement 3. The section on rough-prime classes below gives such a decomposition. It reduces the smooth inputs to explicit collision equations in boundedly many primes, proves that the uncovered proportion tends to zero, and identifies a failure of summing a unit error over every pair of short-slice fixed parts.

Standing and composition. Theorems A and B and the implication (D) ⇒\Rightarrow E0955 have the independent review and separate grade described above; (D) itself remains unproved. G0 has the author-recorded uniform sieve proof linked above; G1 is reduced, in its trimmed form, to Gap G1-core; G2 is the unresolved smooth-input estimate. For every δ\delta, G0 and G1 together with G2 at one fixed η∈(0,1/2)\eta\in(0,1/2) would give (D), because CD(δ)(x)≤2CS1(x)+2CS2(x)C_{D(\delta)}(x)\le2C_{S_1}(x)+2C_{S_2}(x); with the trimmed forms of G1 and G2 they would give statement 3 of Theorem B instead. Theorem B then supplies the image truncation and the density conclusion. Theorem C below replaces this split by rough-prime classes whose collision bounds would give statement 3 without (D). The finite census proves none of G0, G1, G2 or the class bounds. There is no full proof of E0955 here.

The density-zero exclusion route is closed by the independently reviewed Theorem A at its stated source interfaces. Changing which density-zero family is removed cannot reopen it. Allowing an arbitrarily small positive discarded proportion gives the distinct, still-open route of Theorem B; establishing that reformulation does not establish its equivalent asymptotic assertion.

Rough-prime classes

This section gives a decomposition that meets statement 3 of Theorem B directly. Outside a set of at most εx\varepsilon x inputs, every input is a small cofactor times a bounded number of distinct large primes, so G2 becomes a finite family of explicit collision equations. The section describes the estimates needed for these equations and the limitation of summing unit errors over all short slices. Theorem C, the identities and Proposition D below are complete author-recorded arguments, outside the review described above. The full-equation local calculation gives an alternative that can omit every fixed finite list of small prime counts; its remaining gap is the global count G2-full below. The gaps G2-quad, G2-bal and G2-full are open.

Classes. Fix 0<θ<τ<10<\theta<\tau<1 and δ>0\delta>0, and put y=xθy=x^\theta. For n≤xn\le x let b(n)b(n), the product of the prime powers pa ∥ np^a\,\|\,n with p≤yp\le y, be its yy-smooth part, and let e(n)=n/b(n)e(n)=n/b(n) be its yy-rough part. For k≥1k\ge1 let Sk(x)\mathcal S_k(x) be the set of n∈D(δ)∩[1,x]n\in D(\delta)\cap[1,x] with b(n)≤xτb(n)\le x^\tau whose rough part e(n)e(n) is squarefree with exactly kk prime factors. Writing P(b)P(b) for the largest prime factor of bb, with P(1)=1P(1)=1, its members are

n=bP1⋯Pk,P(b)≤xθ<Pk<⋯<P1,b≤xτ,n=bP_1\cdots P_k,\qquad P(b)\le x^\theta<P_k<\dots<P_1,\qquad b\le x^\tau,

and k<1/θk<1/\theta, since xkθ<e(n)≤xx^{k\theta}<e(n)\le x. Since σ(e)/e=∏i(1+1/Pi)≤exp⁡(x−θ/θ)\sigma(e)/e=\prod_i(1+1/P_i)\le\exp(x^{-\theta}/\theta), membership in D(δ)D(\delta) forces s(b)≥δb/2s(b)\ge\delta b/2 for large xx; in particular b≥2b\ge2.

Theorem C. (i) For every xx with xθ≥2x^\theta\ge2, with an absolute implied constant,

#((D(δ)∩[1,x])∖⋃1≤k<1/θSk(x))≤θτ x+O(xτlog⁡x)+2xxθ+xτ.\#\Bigl((D(\delta)\cap[1,x])\setminus\bigcup_{1\le k<1/\theta} \mathcal S_k(x)\Bigr) \le\frac\theta\tau\,x+O\Bigl(\frac{x}{\tau\log x}\Bigr) +\frac{2x}{x^\theta}+x^\tau .

(ii) Suppose that there is τ∈(0,1)\tau\in(0,1) such that for every δ>0\delta>0, every θ∈(0,τ)\theta\in(0,\tau) and every k<1/θk<1/\theta there are KK and x0x_0 with CSk(x)(x)≤KxC_{\mathcal S_k(x)}(x)\le Kx for all x≥x0x\ge x_0. Then every set of natural density zero has a preimage under ss of natural density zero.

Proof. (i) An input n∈D(δ)∩[1,x]n\in D(\delta)\cap[1,x] in no class has b(n)>xτb(n)>x^\tau, or a rough part that is not squarefree, or e(n)=1e(n)=1. Since log⁡b(n)\log b(n) is the sum of log⁡p\log p over the prime powers pj∣np^j\mid n with p≤yp\le y,

∑n≤xlog⁡b(n)=∑p≤ylog⁡p∑j≥1⌊xpj⌋≤x∑p≤ylog⁡pp−1=x (θlog⁡x+O(1))\sum_{n\le x}\log b(n)=\sum_{p\le y}\log p\sum_{j\ge1} \Bigl\lfloor\frac{x}{p^j}\Bigr\rfloor \le x\sum_{p\le y}\frac{\log p}{p-1}=x\,(\theta\log x+O(1))

by Mertens' estimate ∑p≤y(log⁡p)/p=log⁡y+O(1)\sum_{p\le y}(\log p)/p=\log y+O(1), and Markov's inequality bounds the inputs of the first kind by (θ/τ)x+O(x/(τlog⁡x))(\theta/\tau)x+O(x/(\tau\log x)). A rough part that is not squarefree is divisible by p2p^2 for some prime p>yp>y, which happens for at most ∑p>yx/p2≤x/(y−1)≤2x/y\sum_{p>y}x/p^2\le x/(y-1)\le2x/y inputs. If e(n)=1e(n)=1 and b(n)≤xτb(n)\le x^\tau, then n≤xτn\le x^\tau. Every other nn lies in Sk(x)\mathcal S_k(x), with kk the number of prime factors of e(n)e(n).

(ii) Let 0<ε<10<\varepsilon<1. Choose δ\delta with ∏p≤1/δ(1−1/p)<ε/3\prod_{p\le1/\delta}(1-1/p)<\varepsilon/3 and put θ=ετ/3\theta=\varepsilon\tau/3. An input outside D(δ)D(\delta) is 11, a prime, or a composite with no prime factor at most 1/δ1/\delta, because a composite nn with a prime factor p≤1/δp\le1/\delta has s(n)≥n/p≥δns(n)\ge n/p\ge\delta n. The last kind is a union of residue classes modulo ∏p≤1/δp\prod_{p\le1/\delta}p, so for large xx at most (ε/3)x+o(x)(\varepsilon/3)x+o(x) inputs lie outside D(δ)D(\delta). Let ExE_x be the complement in [1,x][1,x] of the union of the classes. By (i), ∣Ex∣≤εx|E_x|\le\varepsilon x for large xx. There are at most 1/θ1/\theta classes, and (r1+⋯+rL)2≤L(r12+⋯+rL2)(r_1+\dots+r_L)^2\le L(r_1^2+\dots+r_L^2) gives

C[1,x]∖Ex(x)≤1θ∑1≤k<1/θCSk(x)(x)≤Kθ2 xC_{[1,x]\setminus E_x}(x)\le\frac1\theta\sum_{1\le k<1/\theta} C_{\mathcal S_k(x)}(x)\le\frac{K}{\theta^2}\,x

for large xx, with KK the largest of the finitely many class constants. This is statement 3 of Theorem B. □\square

Since Sk(x)⊆D(δ)\mathcal S_k(x)\subseteq D(\delta) and CSC_S increases with SS, (D) for every δ\delta implies the hypothesis of (ii). The converse is not shown, and the hypothesis of (ii) is not shown to follow from the problem. The logarithmic prime sum in (i) has an elementary proof. The Chebyshev bound established in the sieve argument gives ∑pj≤Nlog⁡p≪N+Nlog⁡N≪N\sum_{p^j\le N}\log p\ll N+\sqrt N\log N\ll N. For an integer N≥2N\ge2, counting prime factors in N!N! and replacing each floor by its argument gives

log⁡N!=∑pj≤N⌊Npj⌋log⁡p=N∑pj≤Nlog⁡ppj+O(N).\log N!=\sum_{p^j\le N}\Bigl\lfloor\frac{N}{p^j}\Bigr\rfloor\log p =N\sum_{p^j\le N}\frac{\log p}{p^j}+O(N).

Integral bounds give log⁡N!=Nlog⁡N−N+O(log⁡N)\log N!=N\log N-N+O(\log N), and ∑p,j≥2(log⁡p)/pj=∑p(log⁡p)/(p(p−1))<∞\sum_{p,j\ge2}(\log p)/p^j=\sum_p(\log p)/(p(p-1))<\infty. This proves the stated logarithmic prime sum, also for real yy by taking N=⌊y⌋N=\lfloor y\rfloor. Thus the only external asymptotic input of Theorem C is Mertens' product theorem. The reduction fixes the shape of the inputs that need collision bounds and proves none of those bounds.

The class equations. For n=bP1⋯Pk∈Sk(x)n=bP_1\cdots P_k\in\mathcal S_k(x), multiplicativity of σ\sigma gives

s(n)=σ(b)∏i≤k(Pi+1)−b∏i≤kPi,s(n)=\sigma(b)\prod_{i\le k}(P_i+1)-b\prod_{i\le k}P_i ,

an equation of degree kk in the primes whose coefficients σ(b)\sigma(b) and bb are at most xτ+o(1)x^{\tau+o(1)}. For pairwise coprime d,e1,e2d,e_1,e_2, expanding s(de)=σ(d)σ(e)−des(de)=\sigma(d)\sigma(e)-de gives the exact identity

s(de1) s(de2)=s(d) s(de1e2)+d σ(d) s(e1) s(e2).s(de_1)\,s(de_2)=s(d)\,s(de_1e_2)+d\,\sigma(d)\,s(e_1)\,s(e_2).

Put Xi=s(bPi)=s(b)Pi+σ(b)X_i=s(bP_i)=s(b)P_i+\sigma(b). Since s(P)=1s(P)=1 for a prime PP, the identity with d=bd=b, e1=P1e_1=P_1 and e2=P2e_2=P_2 gives the two-prime identity

s(b) s(bP1P2)=X1X2−b σ(b).s(b)\,s(bP_1P_2)=X_1X_2-b\,\sigma(b).

With e1=P1e_1=P_1 and e2=P2P3e_2=P_2P_3 instead, the two-prime identity for P2P3P_2P_3 and s(b)(P2+P3+1)=X2+X3−2σ(b)+s(b)s(b)(P_2+P_3+1)=X_2+X_3-2\sigma(b)+s(b) give

s(b)2 s(bP1P2P3)=X1X2X3−b σ(b)(X1+X2+X3)+b σ(b)(2σ(b)−s(b)).s(b)^2\,s(bP_1P_2P_3)=X_1X_2X_3-b\,\sigma(b)(X_1+X_2+X_3) +b\,\sigma(b)\bigl(2\sigma(b)-s(b)\bigr).

So inside S1\mathcal S_1 a collision is a linear equation in two primes. Inside S2\mathcal S_2 it is the split quaternary quadric

s(b′)X1X2−s(b)X1′X2′=s(b′) b σ(b)−s(b) b′σ(b′)s(b')X_1X_2-s(b)X_1'X_2'=s(b')\,b\,\sigma(b)-s(b)\,b'\sigma(b')

in four variables of the form s(b)P+σ(b)s(b)P+\sigma(b). Inside S3\mathcal S_3 it is a cubic in six such variables, and inside Sk\mathcal S_k an equation of degree kk in 2k2k primes.

Full equations with at least three primes per input. The local-density argument gives a possible replacement for the linear and quadratic slices. Fix 0<β<1/20<\beta<1/2. The number of prime divisors of a uniform n≤xn\le x in (xθ,xβ](x^\theta,x^\beta] has mean M=log⁡(β/θ)+o(1)M=\log(\beta/\theta)+o(1) and variance at most M+o(1)M+o(1), by expanding its first two moments. Thus, for every fixed K<MK<M, the proportion of inputs with at most KK prime factors above xθx^\theta is at most (M+o(1))/(M−K)2(M+o(1))/(M-K)^2. This proportion tends to zero as θ→0\theta\to0. Theorem C's proof therefore still reaches Theorem B(3) if its class estimates are required only for k≥3k\ge3: the small-kk classes can be included in the discarded proportion.

For b,b′≤y=xτb,b'\le y=x^\tau, the linked page removes a set of reciprocal weight o(log⁡y)o(\log y) so that vp(σ(b))>vp(b)v_p(\sigma(b))>v_p(b) for p≤Wp\le W and p∤(b,σ(b))p\nmid(b,\sigma(b)) for p>Wp>W, where W=log⁡log⁡y/(4log⁡log⁡log⁡y)W=\log\log y/(4\log\log\log y), and likewise for b′b'. This removes o(x)o(x) class inputs. Let ρpr(b,b′)\rho_{p^r}(b,b') be prp^r times the probability that the two class polynomials agree modulo prp^r when their 2k2k variables are independent units. For k≥3k\ge3 the page proves

ρpr(b,b′)=1+Ok(p−2)(p>k, p∤bσ(b)b′σ(b′))\rho_{p^r}(b,b')=1+O_k(p^{-2}) \quad\bigl(p>k,\ p\nmid b\sigma(b)b'\sigma(b')\bigr)

uniformly in rr, and ρpr≤1+Ok(p−1)\rho_{p^r}\le1+O_k(p^{-1}) at every prime where each coefficient pair is primitive. At a small prime, unequal valuations of b,b′b,b' prevent an integer collision; equal valuations ee give sup⁡rρpr=pep/(p−1)\sup_r\rho_{p^r}=p^e p/(p-1). The corresponding local majorant Uk(b,b′)\mathfrak U_k(b,b'), defined there using these suprema and set to zero for incompatible small-prime valuations, satisfies

∑b,b′ retainedUk(b,b′)bb′≪klog⁡2y.\sum_{b,b'\ {\rm retained}}\frac{\mathfrak U_k(b,b')}{bb'} \ll_k\log^2y.

The continuous output density obtained by weighting each prime variable with dP/log⁡PdP/\log P is Oδ,θ,k(1/(blog⁡x))O_{\delta,\theta,k}(1/(b\log x)). On any fixed output interval [0,Cx][0,Cx], the local majorants times the overlaps of these densities therefore have total O(x)O(x).

Gap G2-full. Bound the off-diagonal prime solutions of the full class equations by these local and continuous majorants with aggregate error O(x)O(x), uniformly over the growing cofactors and the prime boxes. The diagonal contributes at most xx. The proved local average does not control this error. The full leading homogeneous form has a singular locus of codimension four regardless of kk, even though the affine critical points at the coefficient-free primes are isolated. Thus increasing the number of free prime variables supplies no automatic point-counting theorem. With G2-full for all the retained classes, Theorem C, the small-kk removal and Theorem B would finish the whole target without G1-core or G2-quad. No such global estimate is proved here.

Slices. Assume τ<1/2\tau<1/2 from here on; Theorem C(ii) allows any τ∈(0,1)\tau\in(0,1). For a pair (n,n′)(n,n') in one class and 1≤j≤k1\le j\le k, the jj-slice fixes the parts d=n/(P1⋯Pj)d=n/(P_1\cdots P_j) and d′=n′/(P1′⋯Pj′)d'=n'/(P_1'\cdots P_j') and leaves the jj largest primes of each input free. The colliding pairs with given fixed parts are the prime solutions of the class equation with bb replaced by dd and kk by jj, the free primes exceeding P(d)P(d) and P(d′)P(d') respectively. There are about x/dx/d free jj-tuples on one side and x/d′x/d' on the other, up to logarithmic factors, and the common value has size about xx. A heuristic count, not a proved estimate, therefore gives about x/(dd′)x/(dd') solutions for each pair of fixed parts, before logarithmic and local factors. Any bound for a class obtained by bounding each pair of fixed parts separately, with an error of at least one per pair, is at least the number of such pairs.

  • The linear slice, j=1j=1, is the S1 computation with cofactors m=dm=d and m′=d′m'=d', with two changes. When h=0h=0 a collision with P≠P′P\ne P' forces P∣s(m′)P\mid s(m'), and a form vanishing identically modulo pp allows only P=pP=p or P′=pP'=p; these cases give O(log⁡x)O(\log x) solutions per pair of fixed parts and need a count of their own, which is not made here. Otherwise the G0 argument, with a sieve exponent smaller than θ/2\theta/2, bounds a pair of fixed parts when mm′≤x1−ϵmm'\le x^{1-\epsilon}, because the parameter interval then has length at least xϵg/(1+log⁡x)x^{\epsilon}g/(1+\log x), and the analogue of G1 over the range mm′≤x1−ϵmm'\le x^{1-\epsilon} sums those bounds. Every pair in S1\mathcal S_1 is of this kind, with mm′≤x2τmm'\le x^{2\tau}.
  • The quadratic slice, j=2j=2, is the quaternary quadric with bb replaced by dd. When P2P2′≤x1−ϵ/(dd′)P_2P_2'\le x^{1-\epsilon}/(dd'), fixing P2P_2 and P2′P_2' too reduces the pair to the linear slice. Otherwise each free prime lies within a factor xϵdd′x^{\epsilon}\sqrt{dd'} of x/d\sqrt{x/d} or of x/d′\sqrt{x/d'}, on its own side. When the right side vanishes, for example when d=d′d=d', the quadric becomes s(d′)X1X2=s(d)X1′X2′s(d')X_1X_2=s(d)X_1'X_2', whose solutions include the diagonal and the coincidences between products of two such variables.
  • The full slice, j=kj=k, leaves only bb and b′b' fixed, so dd′≤x2τdd'\le x^{2\tau} and the heuristic count per pair is large, but the equation has degree kk in 2k2k primes.

Gap G2-quad. An upper bound of the heuristic order for the prime solutions of the quaternary quadric, uniform in fixed parts with dd′≤xγdd'\le x^{\gamma} for some fixed γ>0\gamma>0 and with congruence conditions sufficient for a four-dimensional upper-bound sieve, together with the matching average of its local factors and a count of the vanishing-right-side components. With τ<γ/2\tau<\gamma/2, G0, the G1 analogue for pairs that reduce to the linear slice, and a bound for that slice's exceptional prime cases, it would settle S2\mathcal S_2, whose pairs all have dd′≤x2τdd'\le x^{2\tau}. None of these is proved here. A count of points on a quaternary quadric with error a power below its main term, such as a delta-method estimate, is a natural tool, but no uniform version has been checked against these coefficients and boxes. The right side is Δ(d,d′)=dσ(d)s(d′)−d′σ(d′)s(d)\Delta(d,d')=d\sigma(d)s(d')-d'\sigma(d')s(d), the integer that governs large common divisors in the large-prime average. Its Lemma 5 shows that Δ(d,d′)=0\Delta(d,d')=0 forces d=d′d=d' when both fixed parts satisfy vp(σ(d))>vp(d)v_p(\sigma(d))>v_p(d) for p≤Wp\le W, have (d,σ(d))(d,\sigma(d)) free of primes above WW, and have the same part supported on primes up to WW. Fixed parts failing these conditions are not covered.

Proposition D (the cost of summing errors over all short slices). Let J≥1J\ge1 and k≥2Jk\ge2J, put α=1/(k+1/2)\alpha=1/(k+1/2), and fix ι>0\iota>0 with kα(1+ι)<1k\alpha(1+\iota)<1; then c′=1−2Jα(1+ι)>0c'=1-2J\alpha(1+\iota)>0. Let Bk(x)B_k(x) be the set of n=mp1⋯pkn=mp_1\cdots p_k with x/2<n≤xx/2<n\le x, mm even and p1,…,pkp_1,\dots,p_k distinct primes in (xα,xα(1+ι)](x^\alpha,x^{\alpha(1+\iota)}]. Then Bk(x)⊆D(1/2)B_k(x)\subseteq D(1/2) and #Bk(x)≥(ck−o(1))x\#B_k(x)\ge(c_k-o(1))x with ck=(log⁡(1+ι))k/(4⋅k!)c_k=(\log(1+\iota))^k/(4\cdot k!). For every j≤Jj\le J, every jj-slice fixed part of a member of Bk(x)B_k(x) exceeds x(1+c′)/2/2x^{(1+c')/2}/2, so every pair of them has dd′>x1+c′/4dd'>x^{1+c'}/4, and for large xx these fixed parts form at least (ck/2)2x1+c′(c_k/2)^2x^{1+c'} pairs.

Proof. Since α>1/(k+1)\alpha>1/(k+1), every such nn has m≤x1−kα<xαm\le x^{1-k\alpha}<x^\alpha, so p1,…,pkp_1,\dots,p_k are exactly the prime factors of nn above xαx^\alpha and the representation is unique. For p1>⋯>pkp_1>\dots>p_k the jj-slice fixed part is d=n/(p1⋯pj)>x1−jα(1+ι)/2≥x(1+c′)/2/2d=n/(p_1\cdots p_j)>x^{1-j\alpha(1+\iota)}/2\ge x^{(1+c')/2}/2. An even composite nn has s(n)≥n/2s(n)\ge n/2. Counting the even mm in (x/(2p1⋯pk), x/(p1⋯pk)](x/(2p_1\cdots p_k),\,x/(p_1\cdots p_k)],

#Bk(x)≥x4∑p1<⋯<pk1p1⋯pk−π(xα(1+ι))k,\#B_k(x)\ge\frac x4\sum_{p_1<\dots<p_k}\frac1{p_1\cdots p_k} -\pi\bigl(x^{\alpha(1+\iota)}\bigr)^k ,

where Mertens' theorem gives $\sum_{x^\alpha<p\le x^{\alpha(1+\iota)}}1/p =\log(1+\iota)+o(1)$, the distinctness condition costs o(1)o(1) because ∑p>xαp−2→0\sum_{p>x^\alpha}p^{-2}\to0, and the subtracted term is at most xkα(1+ι)=o(x)x^{k\alpha(1+\iota)}=o(x). A fixed part determines nn up to the choice of p1,…,pjp_1,\dots,p_j, so for large xx there are at least (ck/2) x1−jα(1+ι)≥(ck/2) x(1+c′)/2(c_k/2)\,x^{1-j\alpha(1+\iota)}\ge(c_k/2)\,x^{(1+c')/2} distinct fixed parts, and at least (ck/2)2x1+c′(c_k/2)^2x^{1+c'} pairs. □\square

So for j≤Jj\le J the members of BkB_k have heuristic count below 4x−c′+o(1)4x^{-c'+o(1)} for every pair of jj-slice fixed parts, and those pairs exceed xx in number by a power. A summation that charges an error of at least one to every pair of represented fixed parts therefore cannot bound their collisions by O(x)O(x). This does not count how many pairs remain after additional arithmetic eliminations: such eliminations require their own argument. Their positive density means that they cannot be deleted once ε<ck\varepsilon<c_k. For δ≤1/2\delta\le1/2 and θ<α\theta<\alpha, a member of BkB_k outside the exceptions of Theorem C(i) lies in Sk′(x)\mathcal S_{k'}(x) for some k′≥kk'\ge k, and its jj largest primes are still p1,…,pjp_1,\dots,p_j. Those exceptions number at most (θ/τ)x+o(x)(\theta/\tau)x+o(x) and there are fewer than 1/θ1/\theta classes, so once θ/τ<ck/2\theta/\tau<c_k/2 some class contains at least θckx/3\theta c_kx/3 members of BkB_k, and the counts above apply to them with a factor of order θ2\theta^2. The all-pairs error sum already fails for the linear slices of B2B_2, and for the quadratic slices of BkB_k with k≥4k\ge4. A proof confined to separate slice bounds with such an error must allow arbitrarily large slice degree as ε→0\varepsilon\to0. Proposition D concerns only that summation rule. It does not show that the collisions of BkB_k are numerous, and it does not exclude other arguments.

Gap G2-bal. Bound the collisions of inputs whose large primes are comparable, such as BkB_k for k≥4k\ge4, by an argument that does not bound each pair of short-slice fixed parts separately. Two forms of the missing input are visible.

  • Detect slice solutions on average. With Q=P+1Q=P+1 and Q′=P′+1Q'=P'+1, the identity s(mP)=m+(P+1)s(m)s(mP)=m+(P+1)s(m) turns a collision of n=mPn=mP and n′=m′P′n'=m'P' into s(m)Q−s(m′)Q′=m′−ms(m)Q-s(m')Q'=m'-m. With g=gcd⁡(s(m),s(m′))g=\gcd(s(m),s(m')), a solution requires g∣m′−mg\mid m'-m and Q≡((m′−m)/g) (s(m)/g)−1Q\equiv((m'-m)/g)\,(s(m)/g)^{-1} modulo s(m′)/gs(m')/g, with Q−1Q-1 a prime at most x/mx/m and Q′−1Q'-1 prime. When s(m′)/g>x/m+1s(m')/g>x/m+1, QQ is the least positive residue of that class. For cofactors of size about x1/2+κx^{1/2+\kappa} with small gg, the residue must fall in an interval of relative length about x−2κx^{-2\kappa}. An approach using a Fourier majorant of this interval and uniform termwise bounds would seek exponential sums of these residues over pairs of cofactors, at frequencies up to about x2κx^{2\kappa}, with a saving of about x2κx^{2\kappa} and with both prime conditions. This is a sufficient route to the expected count, not a necessary bound on each frequency. A bound saving a fixed small power reaches only cofactors slightly above x1/2x^{1/2}. The inputs BkB_k have cofactors near x1−αx^{1-\alpha}, so κ\kappa is near 1/2−α1/2-\alpha. With M≈x1−αM\approx x^{1-\alpha} cofactors on each side they need a saving of about x1−2α=M(1−2α)/(1−α)x^{1-2\alpha}=M^{(1-2\alpha)/(1-\alpha)} in sums of about M2M^2 terms, close to square-root cancellation when kk is large. These are Kloosterman fractions whose numerator, inverse and modulus are all arithmetic functions of the cofactors. No estimate for them is proved here.
  • A level of distribution beyond x1/2x^{1/2}. Counting one input's largest prime with a sieve and its partners through the residues of s(n′)s(n') needs the values s(n′)s(n') in progressions to moduli s(m)es(m)e of size about x1−αx^{1-\alpha} or more when that input lies in BkB_k. The same holds when the two-prime identity turns one side into a divisor count, with moduli of size about bx\sqrt{bx} or larger. A collision bound gives such distribution through the large sieve only on average over moduli up to about x1/2x^{1/2}, and for general sequences the large sieve cannot do better. In outline, an Elliott–Halberstam-type estimate for the values of ss, with explicit local main terms, would bound every pair whose first cofactor is at most x1−2ϵx^{1-2\epsilon}. Its main term would need only the local densities of s(n′)s(n') modulo qq, in place of the pairwise average G1. This outline is not a proved implication: the hypothesis would need an exact formulation, and the repetition of one modulus s(m)es(m)e for many cofactors mm would need its own bound.

The missing estimates concern the distribution at scale one of s(n)s(n) on inputs with several large prime factors of comparable size and none above about x1/2x^{1/2}. They remain unproved here; Proposition D does not refute them. A route that proves tightness without bounding collisions class by class is not affected by Proposition D. Gap G1-core in the large-prime class is the same kind of requirement at the cofactor scale: there the modulus is a common divisor of s(a)s(a) and s(a′)s(a'), and the residue whose least representative must rarely lie in a short initial interval is −σ(c)s(c)−1-\sigma(c)s(c)^{-1}. In both places Brun–Titchmarsh-type counting works exactly when some free prime has a range longer than the modulus.

The averaged sieve error, with its weights retained. There is a precise form of the first proposed estimate. Fix a rough-prime class Sk(x)\mathcal S_k(x) and write each member uniquely as mPmP, where PP is its largest prime. For a fixed eligible mm, the allowed PP form the primes in an interval ImI_m: the conditions P>max⁡{xθ,P(m)}P>\max\{x^\theta,P(m)\} and mP≤xmP\le x are interval conditions, and s(mP)≥δmPs(mP)\ge\delta mP supplies at most another upper endpoint. The remaining class conditions depend only on mm. For large xx, every such cofactor has s(m)≥δm/2s(m)\ge\delta m/2.

Consider the pairs m≠m′m\ne m' with h=σ(m′)−σ(m)≠0h=\sigma(m')-\sigma(m)\ne0, g∣hg\mid h, and two primitive, locally admissible forms P=u+βtP=u+\beta t, P′=v+λtP'=v+\lambda t, where g=(s(m),s(m′))g=(s(m),s(m')), β=s(m′)/g\beta=s(m')/g and λ=s(m)/g\lambda=s(m)/g. Call these the regular pairs. Let Jm,m′J_{m,m'} be their actual parameter interval, of length ℓm,m′≤xg/(ms(m′))\ell_{m,m'}\le xg/(m s(m')), with the same endpoint conventions as Im,Im′I_m,I_{m'}. Let fm,m′(t)f_{m,m'}(t) be the product of the forms. The prime-pair count for all other off-diagonal cofactor pairs is denoted Cdeg(x)C_{\rm deg}(x). This count includes the h=0h=0 case and the possible prime values of nonprimitive forms; it is not silently discarded.

Fix 0<κ<θ0<\kappa<\theta and set z=xκz=x^\kappa. Use, for each regular pair, the explicit weights λd(m,m′)\lambda_d^{(m,m')} of the uniform sieve argument, and put

Rq(m,m′)=#{t∈Jm,m′∩Z:q∣fm,m′(t)}−ℓm,m′ωm,m′(q)q,Ez(x)=∑(m,m′)regular ∑d,e<zλd(m,m′)λe(m,m′)R[d,e](m,m′).\begin{aligned} R_q(m,m')&=\#\{t\in J_{m,m'}\cap\mathbb Z:q\mid f_{m,m'}(t)\} -\frac{\ell_{m,m'}\omega_{m,m'}(q)}q,\\ \mathcal E_z(x)&= \sum_{\substack{(m,m')\\\text{regular}}}\ \sum_{d,e<z} \lambda_d^{(m,m')}\lambda_e^{(m,m')}R_{[d,e]}(m,m'). \end{aligned}

The sums on d,ed,e use the squarefree support specified with those weights. They are finite sums of explicitly given real numbers; the remainders and the total Ez\mathcal E_z are signed. All relevant primes exceed zz, so summing the finite sieve inequality gives, for an absolute constant CC,

CSk(x)(x)≤x+Cdeg(x)+Cxδκ2log⁡2x∑(m,m′)regularg Sx(m,m′)mm′+Ez(x).C_{\mathcal S_k(x)}(x) \le x+C_{\rm deg}(x)+ \frac{Cx}{\delta\kappa^2\log^2x} \sum_{\substack{(m,m')\\\text{regular}}} \frac{g\,\mathfrak S_x(m,m')}{mm'}+\mathcal E_z(x).

The xx term covers equal cofactors, which force P=P′P=P'. The main term uses only the proved denominator bound and the comparison of singular series cutoffs. It is valid even when ℓm,m′<1\ell_{m,m'}<1; unlike G0, it does not absorb the remainders individually. Consequently, a O(log⁡2x)O(\log^2x) bound for the displayed local-factor sum, Cdeg(x)=O(x)C_{\rm deg}(x)=O(x) and the upper bound Ez(x)≤Kx\mathcal E_z(x)\le Kx for some fixed KK would prove the class estimate in Theorem C. The constants may depend on δ,θ,τ,k,κ\delta,\theta,\tau,k,\kappa. None of these three bounds for general rough-prime classes is established here. Bounding each ∣Rq∣|R_q| by ω(q)\omega(q) and summing absolute weights produces an error majorant of at least one per regular pair, from d=e=1d=e=1. Proposition D explains why charging that bound to every represented cofactor pair cannot work; a reduction to regular pairs must quantify which pairs it removes. Merely displaying the signed sum supplies no cancellation. Its explicit weights specify an analytic estimate to attack without assuming that the residues are independent.

Other whole-target attempts and their failure points. The proof of Pollack, Pomerance and Thompson's finite-target theorem (2017 manuscript, Section 2, pp. 3–4) writes n=den=de with dd the largest divisor below x\sqrt x. For fixed output aa, the identity a=σ(d)s(e)+s(d)ea=\sigma(d)s(e)+s(d)e determines s(e)s(e) modulo s(d)/(d,σ(d))s(d)/(d,\sigma(d)). Its count is a bound for each output; multiplying that bound by the number of targets retains the square-root restriction. Averaging it without a new estimate for which residues actually occur does not give Theorem B(4).

Luca and Pomerance's positive-density range theorem (15-page preprint, Section 3, pp. 6–13) does supply a linear collision bound on selected classes. Its inputs have n=mp∈(x/2,x]n=mp\in(x/2,x] with m≤x7/15m\le x^{7/15}, hence p>x8/15/2p>x^{8/15}/2. Its proof therefore does not bound the positive-density complement in G2. Its further prime ranges are used in the local-factor argument and cannot be removed just by summing cofactor boxes. These two source proofs were read in their transcriptions for the stated uses; no new verification of their external premises or PDF fidelity is asserted.

For a counterexample, the large localized fibers of the same Pollack–Pomerance–Thompson paper (Section 3, pp. 4–6) do not themselves supply positive input density. Common multiplication does not amplify an equal-value fiber into another one: if s(ni)=as(n_i)=a and r>1r>1 is coprime to every nin_i, then

s(rni)=σ(r)a+s(r)ni.s(rn_i)=\sigma(r)a+s(r)n_i.

Since s(r)>0s(r)>0, these values are distinct for distinct nin_i. This exact identity rules out that amplification step only. Different multipliers or another construction are not excluded. No positive-upper-density preimage of a density-zero target is constructed here.

Next discriminating tests

  • Full equations. Gap G2-full can bypass the large-divisor core and the quadratic slice. The prime-power local densities, their reciprocal-weighted cofactor average and the continuous main term are supplied by the full-equation calculation. The missing test is an integer prime-solution estimate for Fσ(b),b,k(P)=Fσ(b′),b′,k(P′)F_{\sigma(b),b,k}(\mathbf P)=F_{\sigma(b'),b',k}(\mathbf P') with k≥3k\ge3, b,b′≤xτb,b'\le x^\tau and all Pi,Pi′>xθP_i,P_i'>x^\theta, whose total error is O(x)O(x) after summing the boxes and cofactors. It must include off-diagonal solutions sharing some prime variables. A count for one fixed b,b′b,b' or one fixed kk does not cover every class needed as the discarded proportion tends to zero. Complete residue counts alone do not bound this error.
  • Large common divisors. Gap G1-core is the first target in the large-prime class. In the core, a divisor dd of s(a)s(a) with d≥P(a)1−κd\ge P(a)^{1-\kappa} has complementary divisor s(a)/d≪c P(a)κlog⁡ys(a)/d\ll c\,P(a)^\kappa\log y, where c=a/P(a)c=a/P(a), so the core partners of aa lie among a+js(a)/λa+js(a)/\lambda for divisors λ\lambda of s(a)s(a) of that size. Enumerating them without using d∣s(a′)d\mid s(a') overshoots log⁡2y\log^2y by about the average number of such λ\lambda, a factor of order log⁡y\log y in a random model. A proof must recover that factor from the condition d∣s(a′)d\mid s(a'), for example by bounding, on average over λ\lambda and jj, the number of aa for which s(a+js(a)/λ)s(a+js(a)/\lambda) is divisible by s(a)/λs(a)/\lambda. Finite sums say little about this regime: W=log⁡log⁡y/(4log⁡log⁡log⁡y)W=\log\log y/(4\log\log\log y) is below 11 unless yy exceeds 10200010^{2000}.
  • Quadratic slice. For cofactors b,b′≤xτb,b'\le x^\tau, count the prime solutions of the quaternary quadric in the balanced box, with the congruence conditions of a four-dimensional upper-bound sieve, and separately its components with vanishing right side. Report the error term against the main term, of order x/(bb′log⁡2x)x/(bb'\log^2x) up to local and doubly logarithmic factors, as bb and b′b' grow. A uniform bound of that order, with G0, the G1 analogue for pairs that reduce to the linear slice, and a bound for that slice's exceptional prime cases, settles S2\mathcal S_2 through G2-quad. It leaves the balanced inputs BkB_k with k≥4k\ge4, so it cannot complete the route.
  • Balanced classes. The first family forcing Proposition D's all-pairs error obstruction for quadratic slices is B4B_4, whose cofactors n/P1n/P_1 lie near x7/9x^{7/9}. For these inputs, seek an upper bound of order xx for the explicit signed remainder Ez(x)\mathcal E_z(x) above, together with the local-factor sum and the degenerate count appearing in the same finite inequality. This states exactly what an averaged use of the linear sieve would need. Fourier estimates for the short residue intervals are one possible tool; uniform bounds on each individual frequency are not necessary. A result for B4B_4 alone would still need extension to every rough-prime class required by Theorem C. No such estimate is supplied here.