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Geometric boundary
Write , , , and . The Haar measures are and . The actual excluded set is
The boundary model below does not alone settle the problem. It does give a sufficient condition for natural density, uniform under common profinite affine transformations of the residues.
Location of a possible logarithmic defect
The ambient measures
on converge weakly to . For a fixed residue class modulo and , harmonic summation between and gives the required mass . Finite unions of such product sets, or approximation of continuous functions by them, prove the assertion.
Replace the sum by its restriction to , obtaining . Every subsequential weak limit has the form
Indeed implies domination of the limit by . Every compact subset of is covered by a fixed finite set of cylinders. Away from , these are all active for large , so the limit agrees with the ambient measure on . No deleted integer lies in ; open-set approximation makes the limit zero there. The slice has zero ambient measure. These observations prove (1).
In particular, a positive discrepancy from requires . If , the analogous ordinary counting argument already gives natural density. Formula (1) locates the possible defect; it does not prove that .
A local reciprocal criterion
Define the closed set
The compatibility condition in the sum is exactly . The complement of is open: a clopen fiber witnessing convergence does so for all its points. On any such fiber, only a reciprocal-summable collection of classes can contribute. The ordinary activated union bound therefore gives finite-periodic approximation on that fiber. In (1), the defect is consequently supported on as well.
Theorem. If , the delayed survivor set has natural density . Convergence is uniform when all residues are changed simultaneously by
Proof. Given , choose a clopen with . The compact set has a finite cover by clopen fibers whose intersecting cylinder families have convergent reciprocal sums. Their union satisfies
The compact set is contained in , so a finite prefix, with moduli at most , covers . Choose such that
Every actual deletion outside the prefix has a witnessing modulus . It cannot lie in , since makes the old covering class there active. If is a period of , then
The bound per class is exact for delayed classes; there is no accumulated inactive-root error. Finite-prefix counting and (4) prove natural density for .
Under (3), transport by . Their measures, periods, cylinder intersections, and reciprocal sums are unchanged. The finite-prefix counting error is uniform over these transformations, as is (4). Thus the conclusion is uniform in .
A noncoherent example with unbounded prime rank
Let be the product of the first odd primes and set . Choose with
The cylinders are pairwise disjoint. For every and every prime , use modulus , with residue modulo and any chosen residue modulo . All moduli are distinct: their -adic valuations distinguish different , and within a fixed the prime distinguishes them. They can therefore be enumerated strictly increasingly.
For a fixed , independent prime coordinates and show that these classes cover almost everywhere. Hence
Moreover
To see this, a point of finite -adic valuation can have a neighborhood meeting only its matching , if there is one. If it is outside that , refine the neighborhood to avoid it too. The last displayed -adic zero set is Haar-null, and is null for each . Thus the theorem gives natural density , uniformly under (3). The reciprocal sum diverges, the survivor density is positive, and both modulus prime rank and pairwise-gcd prime rank are unbounded. The residues need not be coherent.
The geometric argument permits multi-residue families as well, with reciprocal sums counting congruence pairs with multiplicity. The next example shows that its local reciprocal hypothesis is not automatic, even for primitive zero-residue singleton families whose natural density exists.
Positive natural density with : proved obstruction
For every , there is a primitive family of distinct zero-residue moduli such that
and the original delayed survivor set nevertheless has natural density . Thus positive survivor measure, primitivity, and even actual natural-density existence do not force local reciprocal summability on any positive-measure part of the survivor set.
Construction and Haar measure
Choose sufficiently large integers such that
For example, a sufficiently large multiple of works. Choose pairwise disjoint finite prime blocks , all primes in larger than , with
They can be chosen successively, beyond all primes already used, by stopping when the prime reciprocal sum first reaches .
Let consist of all products of distinct primes from , and install the zero class at every . All moduli are distinct and primitive: within a block they are squarefree of the same rank, and different blocks use disjoint prime sets. They therefore admit the required strictly increasing enumeration.
Let and . For Haar-random , let count the primes of dividing . Then , and independent prime coordinates give
Consequently .
Reciprocal divergence in every neighborhood
The reciprocal sum of one block is
To check the approximation, draw primes independently with probabilities . The probability of no collision is . Each draw has maximal point mass at most , so the union bound over pairs gives collision probability . Stirling's formula shows that the right side of (9) tends to infinity. Increase the initial choice of the if necessary so that every block reciprocal sum is at least one.
Fix a modulus . All sufficiently late blocks consist entirely of primes coprime to . For every in these blocks, the cylinder meets every residue fiber modulo , by CRT. Summing (9) over these blocks proves divergence in every fiber. This is exactly . The same observation shows that is dense in . Since is open, , establishing (5).
Uniform counting bound for one block
Fix one block, abbreviating , , and . For an integer , let
and let be the number of primes in this sum. Average over . Exact floor counts imply
Therefore
using and .
If a positive integer is deleted by a modulus in this block, that modulus divides and hence is at most . At most one of its prime factors can exceed . Thus . By (7), for sufficiently large , . Chebyshev's inequality and (10) give the uniform bound
with an absolute constant .
Natural-density conclusion and activation
For zero residues, a positive full hit automatically has , so original activation introduces no exception at all. By (11), the union of blocks after has at most
hits below , uniformly in . For each only finitely many distinct moduli can be active, so this countable union bound follows directly from the finite one. Its normalized upper bound tends to zero as by (6).
Every finite union of blocks is periodic, and its Haar measure tends to as the blocks exhaust the family. The last tail estimate therefore proves natural density for the excluded set and for its complement. This construction is an obstruction to making the local reciprocal criterion automatic, not a counterexample to the target density statement.