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Translation dynamics


This is a different approach from the previous compression and first-kill arguments. It treats the simultaneous translation of every residue as a dynamical parameter. The resulting dichotomy is proved, but neither of its alternatives has been established universally for singleton systems.

The dichotomy

Fix a family Cq=[aq]qC_q=[a_q]_q and let G=Z^G=\widehat{\mathbb Z} with Haar probability μ\mu. Put

U=⋃qCq,β=μ(U).U=\bigcup_q C_q,\qquad \beta=\mu(U).

For z∈Gz\in G, translate every residue by zz and retain the original activation thresholds. Thus

Bz={n≥1:∃q≤n, n−z∈Cq},FN(z)=1HN∑n≤Nn∈Bz1n.B_z=\{n\ge1:\exists q\le n,\ n-z\in C_q\},\qquad F_N(z)=\frac1{H_N}\sum_{\substack{n\le N\\n\in B_z}}\frac1n.

Each FNF_N is continuous, indeed locally constant, on GG. Define

Λ=lim sup⁡N→∞max⁡z∈GFN(z).\Lambda=\limsup_{N\to\infty}\max_{z\in G}F_N(z).

Theorem. For Haar-almost every zz, BzB_z has natural density β\beta. For a comeager set of zz (one containing a countable intersection of dense open sets),

lim inf⁡NFN(z)=β,lim sup⁡NFN(z)=Λ.(1)\liminf_N F_N(z)=\beta,\qquad \limsup_N F_N(z)=\Lambda. \tag{1}

Consequently exactly one of the following holds:

  • FN→βF_N\to\beta uniformly over all z∈Gz\in G;
  • the shifts for which logarithmic density fails form a Haar-null, comeager set.

The theorem also permits multiple residues at each modulus. It therefore does not itself capture the singleton restriction needed for Problem 25.

Uniform lower envelope and directed shifts

Write U≤k=⋃q≤kCqU_{\le k}=\bigcup_{q\le k}C_q and βk=μ(U≤k)\beta_k=\mu(U_{\le k}). Every fixed finite delayed prefix has harmonic averages tending to βk\beta_k, uniformly in zz: there are only finitely many translations modulo its common period. Since every BzB_z contains that prefix,

lim inf⁡Nmin⁡zFN(z)≥β.\liminf_N\min_zF_N(z)\ge\beta.

On the other hand, Haar translation invariance gives exactly

∫GFN(z) dμ(z)=1HN∑n≤Nβnn≤β.\int_G F_N(z)\,d\mu(z) =\frac1{H_N}\sum_{n\le N}\frac{\beta_n}{n}\le\beta.

Thus

min⁡zFN(z)⟶β.(2)\min_zF_N(z)\longrightarrow\beta. \tag{2}

In particular every individual lower limit is at least β\beta.

The elementary shift relation is one-sided:

Bz+b⊆Bz+b(b∈Z≥0).B_z+b\subseteq B_{z+b}\qquad(b\in\mathbb Z_{\ge0}).

Indeed a class active at nn is still active at n+bn+b. For any S⊆NS\subseteq\mathbb N,

0≤HS(N)−HS+b(N)≤Hmin⁡(b,N).0\le H_S(N)-H_{S+b}(N)\le H_{\min(b,N)}.

This follows by subtracting the two weights of each n∈Sn\in S; all differences are nonnegative, and their sum over all integers is Hmin⁡(b,N)H_{\min(b,N)}. With H0=0H_0=0, it follows that

FN(z+b)≥FN(z)−HbHN,FN(z−b)≤FN(z)+HbHN.(3)F_N(z+b)\ge F_N(z)-\frac{H_b}{H_N},\qquad F_N(z-b)\le F_N(z)+\frac{H_b}{H_N}. \tag{3}

Only the bound for fixed bb is needed below.

Generic shifts attain the uniform extremes

Fix ε>0\varepsilon>0 and N0N_0. The sets

⋃N≥N0{z:FN(z)>Λ−ε},⋃N≥N0{z:FN(z)<β+ε}(4)\bigcup_{N\ge N_0}\{z:F_N(z)>\Lambda-\varepsilon\},\qquad \bigcup_{N\ge N_0}\{z:F_N(z)<\beta+\varepsilon\} \tag{4}

are open and dense.

To verify density of the first, fix a basic open neighborhood z≡r(modL)z\equiv r\pmod L. For arbitrarily large NN, some zNz_N satisfies FN(zN)>Λ−ε/2F_N(z_N)>\Lambda-\varepsilon/2. There is a positive representative b∈{0,…,L−1}b\in\{0,\ldots,L-1\} for which zN+bz_N+b lies in that neighborhood. For sufficiently large NN, (3) loses less than ε/2\varepsilon/2. This proves density. For the second, choose a minimizer with FN(zN)≤βF_N(z_N)\le\beta, which exists by the integral bound. Move it into the neighborhood using a nonpositive shift of magnitude at most L−1L-1, and use the other inequality in (3).

Baire's theorem, applied to (4) for all integer N0N_0 and positive rational ε\varepsilon, now proves (1). The reverse inequalities follow from (2) and the definition of Λ\Lambda. If Λ=β\Lambda=\beta, (2) and the uniform upper envelope give uniform convergence. If Λ>β\Lambda>\beta, the comeager set in (1) consists of irregular shifts.

Almost every shift: an elementary maximal argument

No pointwise ergodic theorem is needed for the measure assertion. We use the following periodic maximal inequality. If g≥0g\ge0 is periodic with period LL and mean mm, then the proportion of starting residues aa for which

sup⁡N≥11N∑n=0N−1g(a+n)>ε\sup_{N\ge1}\frac1N\sum_{n=0}^{N-1} g(a+n)>\varepsilon

is at most 2m/ε2m/\varepsilon.

If m>εm>\varepsilon this is immediate. Otherwise any witnessing interval can be reduced modulo LL to one of length at most LL, still with mean greater than ε\varepsilon. For the bad starting positions in one period, greedily select the leftmost uncovered starting position aa and one such half-open interval [a,a+ℓ)[a,a+\ell). The selected intervals are disjoint, cover all bad starting positions, and lie within [0,2L)[0,2L). Their total length is at most 2Lm/ε2Lm/\varepsilon, which bounds the number of bad starts.

Fix kk and let Vk=U∖U≤kV_k=U\setminus U_{\le k}. Its indicator is the increasing limit of periodic indicators 1U≤j∖U≤k\mathbf1_{U_{\le j}\setminus U_{\le k}}. Strict-threshold maximal events pass to this increasing limit, so

μ{z:sup⁡N1N∑n=1N1Vk(n−z)>ε}≤2(β−βk)ε.(5)\mu\left\{z:\sup_N\frac1N \sum_{n=1}^N\mathbf1_{V_k}(n-z)>\varepsilon\right\} \le\frac{2(\beta-\beta_k)}\varepsilon. \tag{5}

The finite-prefix part of the full trace of UU has density βk\beta_k at every zz. If the full trace has upper density greater than β+ε\beta+\varepsilon, its VkV_k part has upper density greater than ε\varepsilon. Its exceptional measure is therefore bounded by (5) for every kk, hence is zero. Finite prefixes also bound its lower density below by β\beta at every zz.

Thus the full trace of UU has natural density β\beta almost surely. The delayed union lies between its fixed finite delayed prefixes and the full trace, so it has the same density almost surely. This completes the dichotomy proof.

Ordinary integer shifts preserve logarithmic behavior

There is an additional exact obstruction to replacing Haar randomness by a fixed ordinary integer translation. For every fixed zz and integer bb, BzB_z and Bz+bB_{z+b} have the same lower and upper logarithmic densities.

It suffices to prove this for b=1b=1. Let

Dz={q:aq+z≡−1(modq)},D_z=\{q:a_q+z\equiv-1\pmod q\},

and let PzP_z be its minimal generators under divisibility, a primitive set. Any point newly admitted to the deletion set by the earlier activation in Bz+1B_{z+1}, compared with Bz+1B_z+1, must be n=qn=q for some q∈Dzq\in D_z. If a proper divisor d∈Dzd\in D_z divides qq, then n−1=q−1≡−1(modd)n-1=q-1\equiv-1\pmod d and q−1≥dq-1\ge d, so that older class already deletes n−1n-1. Consequently

Bz+1∖(Bz+1)⊆Pz.B_{z+1}\setminus(B_z+1)\subseteq P_z.

Primitive sets have logarithmic density zero by the established multiples theorem, and physical translation by one changes the harmonic sum by at most one. Hence FN(z+1)−FN(z)→0F_N(z+1)-F_N(z)\to0. Iteration proves the assertion for any fixed integer bb.

Thus, if one center is exceptional, its entire dense integer orbit is exceptional. Almost-everywhere regularity cannot repair it by choosing a fixed integer shift.

What this changes, and what it does not

For a fixed family, it is enough for a negative construction to find arbitrarily late translated finite-prefix peaks with a fixed excess over β\beta. The centers need not be compatible between peaks: (3) and Baire's theorem produce one center exhibiting oscillation. The missing condition is still a positive normalized harmonic excess, not a bounded finite anomaly.

In particular, any original excess ld⁡‾(B0)>β\overline{\operatorname{ld}}(B_0)>\beta produces an oscillating common profinite translate of the same entire family. Unlike the earlier subfamily extraction, this preserves all moduli and all compatibility relations between the full cylinders, as well as their Haar union measure.

Conversely, proving existence at every common profinite shift of one family would automatically prove uniform convergence over those shifts. Almost-sure existence is much weaker: it holds even for multi-residue families and allows a comeager exceptional set.

No uniform upper bound Λ≤β\Lambda\le\beta has been obtained for arbitrary singleton families. The finite-sharp counterexamples have only bounded harmonic excess and do not supply the peaks required here.

The same dichotomy also holds for ordinary counting averages: replace FNF_N by ∣Bz∩[1,N]∣/N|B_z\cap[1,N]|/N and Hb/HNH_b/H_N in (3) by b/Nb/N.