Wiki
Wiki

Research notes on every problem, and a library of the papers behind them. Built from the open erdos repository.

Updated

Weighted divisibility moments


These are proved estimates, not a resolution of Problem 25. They remove the overlap hypothesis from the parent-refinement obstruction on a substantial, but bounded, range of sampling scales.

A weighted version of harmonic domination

Let W:N→[0,∞)W:\mathbb N\to[0,\infty) depend only on divisibility by a fixed finite set of primes, and suppose that WW is nondecreasing under divisibility. Regard the same function as a function on Z^\widehat{\mathbb Z}, with Haar measure μ\mu. Then

∑n≤XW(n)n≤H⌊X⌋∫W dμ.(1)\sum_{n\le X}\frac{W(n)}n \le H_{\lfloor X\rfloor}\int W\,d\mu. \tag{1}

Here the stated prime-divisibility dependence means that only the indicators 1p∣n\mathbf1_{p\mid n}, not unbounded valuations, are used. Thus WW is bounded. Each superlevel set {W>t}\{W>t\} is a multiples set generated by finitely many squarefree divisors of the product of the chosen primes. Apply the exact multiples harmonic inequality from basic reductions to every superlevel, and integrate in tt. This proves (1).

The parent weights

Use the notation of the parent-refinement note:

P={p:3≤p≤z},λ=∑p∈P1p,r=⌊2λ−6λ⌋,b=⌈2λ+2λ⌉,s=b−r.\mathcal P=\{p:3\le p\le z\},\quad \lambda=\sum_{p\in\mathcal P}\frac1p,\quad r=\lfloor2\lambda-6\sqrt\lambda\rfloor,\quad b=\lceil2\lambda+2\sqrt\lambda\rceil,\quad s=b-r.

All assertions below concern sufficiently large λ\lambda. Put

Pn=∏p∈Pp∣n(1−2/p)−1,c0=2log⁡2−1,κ=2+c0=1+2log⁡2.P_n=\prod_{\substack{p\in\mathcal P\\p\mid n}}(1-2/p)^{-1}, \qquad c_0=2\log2-1, \qquad \kappa=2+c_0=1+2\log2.

For either a=1/2a=1/2 or a=1a=1, (1) and a weighted Chernoff bound give

1H⌊X⌋∑n≤XωP(n)≥rPnan≤exp⁡{−c0λ+O(λ)}.(2)\frac1{H_{\lfloor X\rfloor}} \sum_{\substack{n\le X\\\omega_{\mathcal P}(n)\ge r}} \frac{P_n^a}{n} \le \exp\{-c_0\lambda+O(\sqrt\lambda)\}. \tag{2}

Indeed W(n)=Pna1ωP(n)≥rW(n)=P_n^a\mathbf1_{\omega_{\mathcal P}(n)\ge r} is divisibility-monotone. With independent Bernoulli variables IpI_p of parameters 1/p1/p, its Haar expectation is at most

2−r∏p∈P(1−1p+2p(1−2/p)−a).2^{-r}\prod_{p\in\mathcal P} \left(1-\frac1p+\frac2p(1-2/p)^{-a}\right).

For each of the two fixed values of aa, the logarithm of the local factor is 1/p+O(p−2)1/p+O(p^{-2}), with an absolute summable error, including the prime 3. The product is consequently exp⁡{λ+O(1)}\exp\{\lambda+O(1)\}. Substituting the definition of rr proves (2), uniformly in XX.

An overlap-free protected-trace bound

Consider arbitrary distinct singleton moduli qq, each prescribing 0 or 1 at at least rr primes of P\mathcal P. Write

T={n:#{p∈P:n mod p∈{0,1}}≤b},B=⋃q{aq+tq:t≥1},0≤aq<q.T=\{n:\#\{p\in\mathcal P:n\bmod p\in\{0,1\}\}\le b\}, \qquad B=\bigcup_q\{a_q+tq:t\ge1\},\quad 0\le a_q<q.

No preparatory sieve, incremental-footprint hypothesis, or overlap restriction is imposed. Uniformly in this family and X≥2X\ge2,

HT∩B(X)H⌊X⌋≤H⌊X⌋exp⁡{−κλ+O(λlog⁡(2λ))}+exp⁡{−c0λ+O(λlog⁡(2λ))}.(3)\frac{H_{T\cap B}(X)}{H_{\lfloor X\rfloor}} \le H_{\lfloor X\rfloor} \exp\{-\kappa\lambda+O(\sqrt\lambda\log(2\lambda))\} +\exp\{-c_0\lambda+O(\sqrt\lambda\log(2\lambda))\}. \tag{3}

To prove this, discard the classes prescribing successes at more than bb primes, since they miss TT. Let θq=μ(T∣[aq]q)\theta_q=\mu(T\mid[a_q]_q), σX=∑q≤Xθq/q\sigma_X=\sum_{q\le X}\theta_q/q, and H=H⌊X⌋H=H_{\lfloor X\rfloor}. The already-proved dimension-two progression estimate, namely (9) of the parent-refinement note, states

HT∩B(X)H≤CσX+exp⁡{O(λlog⁡(2λ))}H∑q≤XPqq.(4)\frac{H_{T\cap B}(X)}H \le C\sigma_X+ \frac{\exp\{O(\sqrt\lambda\log(2\lambda))\}}H \sum_{q\le X}\frac{\sqrt{P_q}}q. \tag{4}

Its hypotheses concern only these classes and TT, and do not include a multiplicity bound. Formula (2) with a=1/2a=1/2 bounds the second term by the second term in (3).

The same note gives

θq≤VzFsPq,Vz=exp⁡{−2λ+O(1)},Fs=exp⁡{O(λlog⁡(2λ))}.\theta_q\le V_zF_sP_q,\qquad V_z=\exp\{-2\lambda+O(1)\},\qquad F_s=\exp\{O(\sqrt\lambda\log(2\lambda))\}.

Every retained modulus has at least rr prime factors from P\mathcal P. Distinctness permits its reciprocal sum to be bounded by the sum over all integers in (2). Using a=1a=1,

σX≤VzFsHexp⁡{−c0λ+O(λ)}.\sigma_X\le V_zF_s H \exp\{-c_0\lambda+O(\sqrt\lambda)\}.

Substitution in (4) proves (3). In an infinite family only finitely many moduli q≤Xq\le X contribute. The representation t≥1t\ge1 is exactly the original activation n≥qn\ge q; no inactive root has been counted.

For each fixed ε>0\varepsilon>0, (3) tends to zero uniformly when

H⌊X⌋≤exp⁡{(κ−ε)λ}.(5)H_{\lfloor X\rfloor}\le \exp\{(\kappa-\varepsilon)\lambda\}. \tag{5}

Since λ=log⁡log⁡z+O(1)\lambda=\log\log z+O(1), this includes X≤exp⁡((log⁡z)κ−ε)X\le\exp((\log z)^{\kappa-\varepsilon}), after reducing the fixed margin if necessary, and in particular X≤zAX\le z^A for every fixed AA. The elementary two-sided prime reciprocal estimate used here is already established in the earlier notes; the formulation (5) needs no translation to zz.

Thus the preparations with moduli at most zz cannot produce a fixed positive protected harmonic deletion in any fixed polynomial-in-zz epoch, even with unrestricted overlap and without assuming a small incremental footprint. Epochs starting at much larger scales are not excluded.

Improvement of the all-scale bounded-overlap error

The a=1/2a=1/2 case also improves (11) of the parent-refinement note to

HT∩B(X)H≤CσX+exp⁡{−c0λ+O(λlog⁡(2λ))}(X≥2).(6)\frac{H_{T\cap B}(X)}H \le C\sigma_X+ \exp\{-c_0\lambda+O(\sqrt\lambda\log(2\lambda))\} \qquad(X\ge2). \tag{6}

This follows directly from (4); its old cutoff split and Cauchy--Schwarz loss are unnecessary. Combining (6) with that note's unchanged survivor comparison and in-parent multiplicity bound gives

HS∩T∩B(X)H≤Lexp⁡{O(λlog⁡(2λ))}τ+exp⁡{−c0λ+O(λlog⁡(2λ))}.(7)\frac{H_{S\cap T\cap B}(X)}H \le L\exp\{O(\sqrt\lambda\log(2\lambda))\}\tau +\exp\{-c_0\lambda+O(\sqrt\lambda\log(2\lambda))\}. \tag{7}

The stronger error does not remove the multiplicity hypothesis from this all-scale, footprint-sensitive conclusion. Formula (3) does remove it, but only yields a vanishing bound in the range (5).