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One more dimension in the unit-congruence bound
This note improves a universal bound but does not resolve Erdős 963. The notation denotes maximum dissociation dimension, not the minimum size of an inclusion-maximal dissociated subset.
Extension theorem
Theorem. Let be even, and let be a finite set of positive integers in one residue class , where . If , then
The case follows from affine-coherent extraction and congruence transfer. Indeed, if the count fails, extraction gives an affine-coherent -subset, and the transfer lemma makes it coherent and hence dissociated. We prove the remaining case .
Split into its two residue classes modulo . If one is empty, the same transfer argument, now modulo , proves (1). Assume both are nonempty.
Suppose is dissociated and , and put . Every has a ternary representation on . If its coefficient sum is , reduction modulo gives
The only possibilities are and . The former representation is all-plus. In the latter, positivity excludes all-negative representations, leaving exactly one positive and negative coefficients. Thus
At most one value of the second kind is positive. Consequently, if , then . The same assertion holds with the two fibers interchanged.
If both fibers have at least three elements, they therefore have dimension at most . Apply the already proved unit-class bound modulo to each: their total size is at most . It remains to treat a fiber of size one or two.
If , then , so suppose . When , equation (2) shows that every maximum -subset of contains
Deleting lowers the dimension of to at most . Applying the unit-class bound to gives
since .
The singleton fiber
Let . By a circuit we mean a nonzero ternary relation whose support contains no smaller support of a nonzero ternary relation. Consider all circuits on of support size at most .
Every such circuit contained in is balanced: its coefficient sum is divisible by , and its absolute value is at most . A circuit through , oriented as , has at most other coordinates. The same congruence and positivity argument as in (2) gives exactly two possible forms:
If , only the first form is possible. If , the first form is impossible as well: circuit minimality makes its summands dissociated, and adjoining would give a dissociated -set. Thus all circuits through have the same coefficient sum on , namely when and when .
Let be generated by the circuits just considered, and put . Two integer functionals annihilate : the actual weights and the function equal to one on , with
These functionals are rationally independent, since contains at least two distinct weights. Hence . In particular .
The actual odd weights give a character equal to one on every coordinate column. Choose a character . Its values partition into two nonempty classes . Both have dimension at most . For if a dissociated -set lay in , adjoining a point of would produce a circuit of size at most using that point; applying contradicts that relation. For a -set in , apply instead.
The classes are still subsets of the original unit class modulo . The established bound at dimension at most gives . This proves (1).
A recursive universal estimate
For put
where the second term is omitted for . These are the previously proved positive-set bounds: the first follows by applying the binary-tree bound to , and the second is the coherent-support bound.
Set , for , and, for ,
Then every finite positive real set of dimension at most has at most elements, and every finite real set of dimension at most has at most elements.
To prove this, use the established integer realization and divide by the largest common power of two. The resulting positive set has a nonempty odd part. Its even part has dimension at most , because one odd element can be adjoined to every dissociated even subset. Partition the odd part into its unit classes modulo . The theorem bounds each by , since . This proves the second term of (4), and supplies the first. Symmetrization proves the real-set bound.
The first new values are
In particular every -element real set contains a dissociated six-set. This still does not prove the required six-set for every -element real set. Equivalently, the estimate does not give the target positive bound .
The remaining unit-congruence gap begins at . A ternary representation across the two modulo- fibers can then omit a coordinate of a maximum set, and the full-support argument (2), as well as the singleton circuit argument, no longer applies.
Sharpening by the new affine theorem
The subsequent eight-point affine theorem improves the unit-class count, for , to . Thus (4) can be strengthened: keep and for , and replace its recursion by
The proof is the same parity split. The first values are now
In particular every -element real set has a dissociated six-set, but the requested threshold is , still unproved.
The same note proves the unmodified unit-class count through for even , through for even , and through for even . Those additional congruence ranges can further lower the odd-part term at some dimensions; they do not establish the bound for unrestricted odd sets. The concrete endpoint was left unresolved by these arguments; it is settled, with bound , by the grid theorem.
Current strengthened recursion
The later fourteen-point theorem gives the affine bound for . For even the unit-class argument above propagates that same bound through : both dropped classes contribute , and the two-point exception contributes at most . The already proved case follows directly from the affine theorem. The endpoint retains its proved bound fourteen, not thirteen.
Combining these facts with [[research/erdos_963/positive_seven|the sharp positive dimension-three bound]] and the grid theorem gives the following current recursion. Set
and for set
Then for positive sets, and for arbitrary real sets.
For the new starting values, the established odd bounds through dimension four are . The sharp positive bound therefore gives . Splitting an odd dimension-five set modulo four gives at most elements, hence . The grid theorem bounds each modulo-four class of a dimension-six odd set by , so its size is at most and . Each use of the even-part bound is justified by adjoining an odd element after normalization. For , there are odd classes, each bounded by , proving (6).
In particular,
Thus every -element real set has a dissociated six-set, and every -element real set has a dissociated seven-set. The required thresholds and remain unproved.