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Parent refinement overlap


The overlapping preparation produces many protected points in parents of very small conditional survivor measure. The following theorem rules out refining these parents with bounded overlap, at all cutoffs, not only polynomial-length epochs. The later weighted estimates improve its error and remove overlap restrictions up to a quantified cutoff. The last section below also treats arbitrary overlap at every cutoff when the assigned parent leaves only a small prime-factor rank. The unrestricted case remains open.

Statement

Let P={p:3≤p≤z}\mathcal P=\{p:3\le p\le z\}, λ=∑p∈P1/p\lambda=\sum_{p\in\mathcal P}1/p, and, for large λ\lambda, put

r=⌊2λ−6λ⌋,b=⌈2λ+2λ⌉,s=b−r=O(λ).r=\lfloor2\lambda-6\sqrt\lambda\rfloor, \quad b=\lceil2\lambda+2\sqrt\lambda\rceil, \quad s=b-r=O(\sqrt\lambda).

Write

R(x)=#{p∈P:x mod p∈{0,1}},T={R≤b}.R(x)=\#\{p\in\mathcal P:x\bmod p\in\{0,1\}\}, \qquad T=\{R\le b\}.

Let SS be the full survivor set of any finite preparation with squarefree moduli supported on P\mathcal P, prescribing only digits 0 and 1 at those primes. A parent fixes such digits at exactly rr primes. Append classes Cq=[aq]qC_q=[a_q]_q, 0≤aq<q0\le a_q<q, with globally distinct moduli, each refining one chosen assigned parent. Parents here are geometric cylinders, not potentially repeated labels.

Assume the classes assigned to each parent have pointwise multiplicity at most LL on TT. Let U=⋃qCqU=\bigcup_q C_q, τ=μ(S∩U)\tau=\mu(S\cap U), and let BB be the appended union activated at n≥qn\ge q. With c0=2log⁡2−1>0c_0=2\log2-1>0, uniformly for X≥2X\ge2,

HS∩T∩B(X)H⌊X⌋≤Lexp⁡{O(λlog⁡(2λ))}τ+exp⁡{−c0λ/2+O(λlog⁡(2λ))}.(1)\frac{H_{S\cap T\cap B}(X)}{H_{\lfloor X\rfloor}} \le L\exp\{O(\sqrt\lambda\log(2\lambda))\}\tau +\exp\{-c_0\lambda/2+O(\sqrt\lambda\log(2\lambda))\}. \tag{1}

All constants are absolute. In particular, τ≤e−cλ\tau\le e^{-c\lambda} and L=eo(λ)L=e^{o(\lambda)} force the left side to tend to zero uniformly in XX. This includes one refinement per parent, or disjoint refinements within each parent. The protected set GG in the earlier preparation lies in S∩TS\cap T, so (1) applies to its trace.

A dimension-two progression estimate

Define

Vz=∏p∈P(1−2/p),Pq=∏p∈Pp∣q(1−2/p)−1,Fs=∑J⊆P∣J∣≤s∏p∈J2p−2.V_z=\prod_{p\in\mathcal P}(1-2/p),\quad P_q=\prod_{\substack{p\in\mathcal P\\p\mid q}}(1-2/p)^{-1},\quad F_s=\sum_{\substack{J\subseteq\mathcal P\\|J|\le s}} \prod_{p\in J}\frac2{p-2}.

Since ∑p∈P2/(p−2)=2λ+O(1)\sum_{p\in\mathcal P}2/(p-2)=2\lambda+O(1),

Fs≤∑j=0s(2λ+O(1))jj!=exp⁡{O(λlog⁡(2λ))}.(2)F_s\le\sum_{j=0}^s\frac{(2\lambda+O(1))^j}{j!} =\exp\{O(\sqrt\lambda\log(2\lambda))\}. \tag{2}

Let jqj_q count the primes of P\mathcal P dividing qq at which aqa_q has digit 0 or 1. Then jq≥rj_q\ge r. Omit classes with jq>bj_q>b, which do not meet TT. Independence at the primes not dividing qq gives the exact conditional probability

θq:=μ(T∣Cq)=VzPq∑J⊆{p∈P:p∤q}∣J∣≤b−jq∏p∈J2p−2.(3)\theta_q:=\mu(T\mid C_q) =V_zP_q \sum_{\substack{J\subseteq\{p\in\mathcal P:p\nmid q\}\\ |J|\le b-j_q}} \prod_{p\in J}\frac2{p-2}. \tag{3}

In particular VzPq≤θq≤VzPqFsV_zP_q\le\theta_q\le V_zP_qF_s.

We claim that, for W≥1W\ge1,

∑1≤t≤Waq+qt∈T1t≤Cθqlog⁡(2W)+exp⁡{O(λlog⁡(2λ))}Pq.(4)\sum_{\substack{1\le t\le W\\a_q+qt\in T}}\frac1t \le C\theta_q\log(2W) +\exp\{O(\sqrt\lambda\log(2\lambda))\}\sqrt{P_q}. \tag{4}

Use the proved elementary dimension-two upper sieve, and choose an absolute B>B2+2B>B_2+2, where B2B_2 is its length exponent. For Y≤zs+BY\le z^{s+B}, sieve at w=Y1/(s+B)w=Y^{1/(s+B)}. A counted quotient has at most ss successes at primes at most ww not dividing qq. Group by their exact set JJ and their two possible digits. Their product dd is at most wsw^s; the remaining quotient interval has length Y/d≥wBY/d\ge w^B, so the upper sieve applies to the other primes. Summing its bound gives

Nq(Y):=#{1≤t≤Y:aq+qt∈T}≤C(s+B)2PqFsY(log⁡Y)2(5)N_q(Y):=\#\{1\le t\le Y:a_q+qt\in T\} \le C(s+B)^2P_qF_s\frac{Y}{(\log Y)^2} \tag{5}

when w≥3w\ge3. The trivial bound Nq(Y)≤YN_q(Y)\le Y handles the remaining range. To see the factor in (5), the summand for a fixed success set is (Y/d)2∣J∣∏p≤w, p∤qd(1−2/p)(Y/d)2^{|J|}\prod_{p\le w,\,p\nmid qd}(1-2/p). Factor out the complete avoiding product and use (2), ∏3≤p≤w(1−2/p)≪(log⁡w)−2\prod_{3\le p\le w}(1-2/p)\ll(\log w)^{-2}, and log⁡w=log⁡Y/(s+B)\log w=\log Y/(s+B).

For Y≥zs+BY\ge z^{s+B}, instead sieve at w=zw=z, grouping by at most b−jqb-j_q successes. The same divisor sum is now exactly (3), giving

Nq(Y)≤CθqY.(6)N_q(Y)\le C\theta_qY. \tag{6}

Partial summation proves (4): the short-range contribution is bounded using ∫0∞min⁡(1,A/u2) du=2A\int_0^\infty\min(1,A/u^2)\,du=2\sqrt A, with A=C(s+B)2PqFsA=C(s+B)^2P_qF_s; the long range contributes Cθqlog⁡(2W)C\theta_q\log(2W). No assumption is made about extra prime factors or prime powers of qq.

Distinctness controls the remaining arithmetic error

Let

βr=Pr⁡{∑p∈PBernoulli⁡(1/p)≥r}.\beta_r=\Pr\left\{\sum_{p\in\mathcal P} \operatorname{Bernoulli}(1/p)\ge r\right\}.

Chernoff's inequality at parameter log⁡2\log2 gives

βr≤2−r∏p∈P(1+1/p)≤exp⁡{−c0λ+O(λ)}.(7)\beta_r\le2^{-r}\prod_{p\in\mathcal P}(1+1/p) \le\exp\{-c_0\lambda+O(\sqrt\lambda)\}. \tag{7}

Every appended modulus has at least rr prime factors in P\mathcal P. Distinctness and the exact multiples inequality from basic reductions therefore imply

∑q≤X1q≤βrH⌊X⌋.(8)\sum_{q\le X}\frac1q\le\beta_rH_{\lfloor X\rfloor}. \tag{8}

Put σX=∑q≤Xθq/q\sigma_X=\sum_{q\le X}\theta_q/q. Activation represents every hit as aq+qta_q+qt with t≥1t\ge1. Since 1/(aq+qt)≤1/(qt)1/(a_q+qt)\le1/(qt), (4) and the union bound give

HT∩B(X)H⌊X⌋≤CσX+exp⁡{O(λlog⁡(2λ))}H⌊X⌋∑q≤XPqq.(9)\frac{H_{T\cap B}(X)}{H_{\lfloor X\rfloor}} \le C\sigma_X+ \frac{\exp\{O(\sqrt\lambda\log(2\lambda))\}} {H_{\lfloor X\rfloor}} \sum_{q\le X}\frac{\sqrt{P_q}}q. \tag{9}

The elementary bound

Pq≪(log⁡log⁡(3q))2(10)P_q\ll(\log\log(3q))^2 \tag{10}

is uniform. Indeed PqP_q is bounded by a constant times ∏p∣q(1−1/p)−2\prod_{p\mid q}(1-1/p)^{-2}. Split those primes at log⁡(3q)\log(3q). The smaller-prime product is O((log⁡log⁡(3q))2)O((\log\log(3q))^2); the logarithm of the remaining product is O(ω(q)/log⁡(3q))=O(1)O(\omega(q)/\log(3q))=O(1).

Write H=H⌊X⌋H=H_{\lfloor X\rfloor}. If H≤e2λH\le e^{2\lambda}, (8) and (10) bound the last factor in (9) by O((1+λ)βr)O((1+\lambda)\beta_r). If H>e2λH>e^{2\lambda}, use Vz=e−2λ+O(1)V_z=e^{-2\lambda+O(1)}, θq≥VzPq\theta_q\ge V_zP_q, Cauchy--Schwarz, and (8) to get

1H∑q≤XPqq≪eλσXβrH≤CσXβr.\frac1H\sum_{q\le X}\frac{\sqrt{P_q}}q \ll e^\lambda\sqrt{\frac{\sigma_X\beta_r}{H}} \le C\sqrt{\sigma_X\beta_r}.

When σX≤1\sigma_X\le1, these estimates prove

HT∩B(X)H≤CσX+exp⁡{−c0λ/2+O(λlog⁡(2λ))}.(11)\frac{H_{T\cap B}(X)}H \le C\sigma_X+ \exp\{-c_0\lambda/2+O(\sqrt\lambda\log(2\lambda))\}. \tag{11}

When σX>1\sigma_X>1, the same assertion follows from the trivial bound one.

Comparing the low-count region to actual survivors

First discard any appended class with S∩Cq=∅S\cap C_q=\varnothing; this changes no hits on SS. Apply (11) to this retained family, and henceforth let σX\sigma_X denote its raw mass sum. For the union UXU_X of the remaining classes with q≤Xq\le X, we claim

μ(T∩UX)≤Fsμ(S∩UX).(12)\mu(T\cap U_X)\le F_s\mu(S\cap U_X). \tag{12}

Take x∈T∩Cqx\in T\cap C_q. Let JJ be its success primes in P\mathcal P not dividing qq. There are at most ss of them. Change all their digits to arbitrary nonsuccess digits. Every resulting point still lies in CqC_q, and now has no success prime outside qq. It must survive the preparation: a matching preparatory class would use only primes dividing qq, hence would contain all of CqC_q, contrary to the discard step.

Thus the entire nonsuccess fiber at JJ, with all other coordinates fixed, belongs to E=S∩UXE=S\cap U_X. For each fixed JJ, let FJF_J be the set of other-coordinate configurations whose full nonsuccess fiber lies in EE. Expanding these fibers to success digits has measure

μ(FJ)∏p∈J2p≤μ(E)∏p∈J2p−2.\mu(F_J)\prod_{p\in J}\frac2p \le \mu(E)\prod_{p\in J}\frac2{p-2}.

Every point of T∩UXT\cap U_X occurs in one such expanded fiber. Summing over ∣J∣≤s|J|\le s proves (12). All sets here are finite unions of cylinders; no infinite-fiber measurability assertion is needed.

Finally a point of TT belongs to at most (br)\binom br parents: choose their rr primes among its at most bb success primes, after which the digits are forced. The in-parent overlap assumption therefore gives

σX≤L(br)μ(T∩UX)≤L(br)Fsτ.\sigma_X\le L\binom br\mu(T\cap U_X) \le L\binom br F_s\tau.

Both (br)\binom br and FsF_s are exp⁡{O(λlog⁡(2λ))}\exp\{O(\sqrt\lambda\log(2\lambda))\}. Substitute in (11), and note that the retained union covers every point counted on the left of (1). This proves the theorem.

Remaining gap

The progression estimate, raw-mass bound (11), and survivor comparison (12) hold without a multiplicity hypothesis. Only the final passage from σX=∑qμ(T∩Cq)\sigma_X=\sum_q\mu(T\cap C_q) to union measure needs it. Without the scale or residual-rank restrictions proved in the later sections, no estimate removing that overlap loss has been proved. Nor has a construction with enough overlapping refinements and protected active trace been obtained. Therefore this theorem excludes a substantial subclass of the proposed construction, not a general counterexample or a general density theorem.

Arbitrary overlap with bounded residual rank

There is a second all-scale theorem, which replaces the overlap hypothesis by a rank hypothesis. Assign each appended class to one geometric parent C=[a]dC=[a]_d, and suppose

q=dm,Ω(m)≤K.q=dm,\qquad \Omega(m)\le K.

The parent modulus is a squarefree product of exactly rr old primes, and its digits are 0 or 1, as above. Uniformly in X≥2X\ge2, without any overlap bound,

HS∩T∩B(X)H⌊X⌋≤54Kexp⁡{O(λlog⁡(2λ))}τ+exp⁡{−c0λ+O(λlog⁡(2λ))}.(13)\frac{H_{S\cap T\cap B}(X)}{H_{\lfloor X\rfloor}} \le 54^K\exp\{O(\sqrt\lambda\log(2\lambda))\}\tau +\exp\{-c_0\lambda+O(\sqrt\lambda\log(2\lambda))\}. \tag{13}

In particular K=o(λ)K=o(\lambda) and τ≤e−cλ\tau\le e^{-c\lambda}, for fixed c>0c>0, exclude a protected harmonic anomaly at every cutoff. Rank counts prime factors with multiplicity; no restriction on the sizes or identities of the extra primes is imposed.

Retain only classes with q≤Xq\le X, with jq≤bj_q\le b, and with S∩Cq≠∅S\cap C_q\ne\varnothing. Partition the counted active hits disjointly among these classes. Within one assigned parent write qi=dmiq_i=dm_i and let cic_i be the assigned harmonic mass divided by H=H⌊X⌋H=H_{\lfloor X\rfloor}. Put

α=∑ici,θ0=VzPd.\alpha=\sum_i c_i,\qquad \theta_0=V_zP_d.

First suppose H≥e2λH\ge e^{2\lambda}.

For each divisor ee of some mim_i, and v(mode)v\pmod e, let

Se,v=∑i:e∣mi(aqi−a)/d≡v(mode)ci.S_{e,v}=\sum_{\substack{i:e\mid m_i\\ (a_{q_i}-a)/d\equiv v\pmod e}}c_i.

The assigned points in this sum belong to the face [a+dv]de[a+dv]_{de}. They also satisfy n≥qi≥den\ge q_i\ge de, so the face is active. It still prescribes at least the rr parent successes. Apply the progression estimate (4) to this face. Since

Pde≤3KPd,θde≤VzPdeFs,PdH≪VzPd=θ0,P_{de}\le3^K P_d,\quad \theta_{de}\le V_zP_{de}F_s,\quad \frac{\sqrt{P_d}}H\ll V_zP_d=\theta_0,

it gives

Se,v≤Aθ0de,A≤3Kexp⁡{O(λlog⁡(2λ))}.(14)S_{e,v}\le\frac{A\theta_0}{de},\qquad A\le3^K\exp\{O(\sqrt\lambda\log(2\lambda))\}. \tag{14}

If the face forces more than bb successes it contributes zero and needs no sieve estimate. The last displayed bound uses Vz=e−2λ+O(1)V_z=e^{-2\lambda+O(1)} and Pd≥1P_d\ge1.

Every retained class satisfies θqi≥θ0\theta_{q_i}\ge\theta_0. Every nonempty compatible pair intersection has conditional TT-probability at most B0θ0B_0\theta_0, where

B0≤32KFs.B_0\le3^{2K}F_s.

Indeed its modulus is d[mi,mj]d[m_i,m_j], adding at most 2K2K prime factors to the parent, and it forces at least rr successes. An intersection forcing more than bb contributes zero.

On the profinite probability space put

Z=∑idmici1T∩Cqi.Z=\sum_i dm_i c_i\mathbf1_{T\cap C_{q_i}}.

Then EZ≥θ0α\mathbb EZ\ge\theta_0\alpha. Expanding the second moment, using CRT, and writing (mi,mj)=∑e∣(mi,mj)φ(e)(m_i,m_j)=\sum_{e\mid(m_i,m_j)}\varphi(e), gives the upper bound

EZ2≤dB0θ0∑eφ(e)∑vSe,v2≤AB0θ02∑ici∑e∣miφ(e)e≤AB02Kθ02α.(15)\mathbb EZ^2 \le d B_0\theta_0\sum_e\varphi(e)\sum_v S_{e,v}^2 \le A B_0\theta_0^2\sum_i c_i \sum_{e\mid m_i}\frac{\varphi(e)}e \le A B_0 2^K\theta_0^2\alpha. \tag{15}

In the first inequality it is harmless to include pairs compatible modulo ee but incompatible modulo their full gcd. The second inequality is (14), and the last uses ∑e∣mφ(e)/e≤d(m)≤2Ω(m)\sum_{e\mid m}\varphi(e)/e\le d(m)\le2^{\Omega(m)}. Cauchy--Schwarz on the support T∩UCT\cap U_C now gives

α≤54Kexp⁡{O(λlog⁡(2λ))}μ(T∩UC),\alpha\le54^K\exp\{O(\sqrt\lambda\log(2\lambda))\} \mu(T\cap U_C),

where UCU_C is the union assigned to that parent.

Each point of TT lies in at most (br)\binom br geometric parents. Sum the preceding bound over parents and apply (12):

∑Cμ(T∩UC)≤(br)μ(T∩UX)≤(br)Fsτ.\sum_C\mu(T\cap U_C) \le\binom br\mu(T\cap U_X) \le\binom br F_s\tau.

Both new factors are exp⁡{O(λlog⁡(2λ))}\exp\{O(\sqrt\lambda\log(2\lambda))\}. This proves the first term of (13) in the large-cutoff range.

For H<e2λH<e^{2\lambda}, the overlap-free bound (3) of weighted divisibility moments is at most exp⁡{−c0λ+O(λlog⁡(2λ))}\exp\{-c_0\lambda+O(\sqrt\lambda\log(2\lambda))\}, since κ=2+c0\kappa=2+c_0. This proves (13) for the remaining cutoffs. Every counting step retained original activation, and distinctness enters the weighted cutoff for the small-cutoff range. Arbitrary unbounded residual rank and arbitrary overlap together are not covered.