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Branch separated centers
Theorem: proved
Partition a family of globally distinct moduli into blocks , indexed by distinct integers , using the residue throughout , and suppose
Assume there is a fixed integer such that, for every prime and every residue , at most centers satisfy both
Then the delayed union, with the original activation , has logarithmic density equal to its full Haar union measure. It has finite-periodic approximation in upper logarithmic density.
Write , and let be the ordinary harmonic sum. For a finite such system of Haar union measure , and every ,
This is a different extension of the bounded-prime-overlap block theorem: arbitrarily many blocks may use a prime, provided their centers have bounded multiplicity in each first-digit branch.
Corollary. For every fixed , the delayed union for arbitrary normalized residues has logarithmic density if
There is no coherence assumption. In particular the one-sided condition suffices. Modulus one is trivial and can be handled separately.
Choose the representative of smallest absolute value, breaking a possible tie consistently. Then , and (4) gives whenever . In the open interval , a fixed residue modulo has at most integer representatives. Thus (2) holds with that . For the one-sided condition use and .
A one-coordinate inequality
Let have Haar law on . Suppose finitely many nonnegative functions have the following property: for each , there is a constant such that
Suppose each branch modulo has at most assigned functions. Then
To prove this, group the functions by their branch , and write , . If a baseline is zero both sides are zero. Otherwise put . The depressions from the baselines have disjoint supports, so
Apply Hölder within each group of at most factors, padding with constant-one factors when needed, to get (6). This argument allows arbitrary variation within each branch; it does not assume that different centers in the same branch have nested deeper balls.
For a product of prime-coordinate spaces, (6) can be iterated. If a factor satisfies (5) at every coordinate on which it depends, replacing it by preserves (5) at all other coordinates: their pointwise baseline upper bounds survive integration and taking positive roots. The -norm operations commute across independent coordinates. Thus
Factors independent of a coordinate can be taken outside its integral.
Apply the inequality to block survivors
For a finite subsystem put
where . With all other coordinates fixed, is constant outside , and cannot increase on that branch. Classes in not divisible by may make it zero everywhere; this is the zero-baseline case already included. Condition (2) therefore permits (7), giving
For countable systems, exhaust finitely many classes in finitely many blocks and pass to the limit. If the full survivor measure is positive, (8) implies
Exact harmonic control of a signed-center block
For every block satisfying (1), with delayed union ,
For , the block is exactly : every generator exceeds , and its active points are , . Subtracting does not increase the cutoff or decrease a harmonic weight, so (10) follows from the exact multiples inequality.
For , let be the primitive core of . Since , the exact identity is
Indeed, a point divisible by a generator is active unless and there is no proper generator divisor of . These exceptional points are exactly ; any proper generator divisor is at most , and makes its deletion active at .
Each point of has a primitive divisor in . Different points cannot choose the same divisor: every primitive divisor is greater than , whereas the points differ by less than . Hence
Partial summation and the exact multiples inequality again give (10). For integer cutoffs this argument is literal; real cutoffs follow by taking integer parts.
Each fixed signed-center block has finite-periodic logarithmic approximation. For nonnegative centers this is the multiples theorem and fixed translation. For negative centers, primitive sets are logarithmically null, so (11) gives the same conclusion. More explicitly, if is finite, then
whose second term is finite. Finite approximation for multiples therefore transfers to the delayed block.
Finish the density theorem
For , (9)--(10) show that all blocks outside any finite selection have normalized harmonic mass at most the omitted sum of their . This tends to zero as the selection grows. Approximate each of the finitely many retained blocks by finitely many of its congruences. Finite unions preserve upper logarithmic approximation, proving the theorem. Any such finite selection is contained in an original finite initial segment of increasing moduli.
If , finite delayed prefixes already imply natural survivor density zero. For a finite family, summing (10) and using (9) proves (3). One can also write the constant-factor consequence
This follows by splitting at and using monotonicity of .
The theorem makes no assertion of natural density when , and it does not control arbitrary moving residues with unbounded primewise collision multiplicities.
A sharper prime-power overlap criterion
Condition (2) can be weakened. For every block using a prime , put
It suffices that the balls , counted once for each block, have pointwise overlap at most for every prime . The theorem and its finite bound (3) then remain valid with this . Condition (2) implies this criterion, because .
To verify the extension, fix the other coordinates. The block survivor factor is constant outside , and is at most this baseline everywhere. A finite family of -adic balls with overlap at most can be colored using colors so that balls of the same color are disjoint. Indeed, order the balls from larger to smaller, allowing repeated balls; all previously colored balls meeting a new ball contain it. At most such balls exist, so greedy coloring works.
Let be the product of the factors in color , padding with empty products if necessary. Hölder and the disjoint-support inequality used above give
The second inequality applies to the factors within each color. Integration and positive roots preserve the baseline and the suppression property outside each remaining prime's prescribed ball. Thus the coordinate induction proving (7), and all subsequent steps, apply unchanged. Infinite blocks follow by finite truncation: the balls needed for a truncation are contained in the displayed .