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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 d(P)d(P) denotes maximum dissociation dimension, not the minimum size of an inclusion-maximal dissociated subset.

Extension theorem

Theorem. Let q≥4q\ge4 be even, and let OO be a finite set of positive integers in one residue class a(modq)a\pmod q, where gcd⁡(a,q)=1\gcd(a,q)=1. If d(O)≤q+1d(O)\le q+1, then

∣O∣≤2d(O)−1.(1)|O|\le2^{d(O)-1}. \tag{1}

The case d(O)≤qd(O)\le q follows from affine-coherent extraction and congruence transfer. Indeed, if the count fails, extraction gives an affine-coherent (d(O)+1)(d(O)+1)-subset, and the transfer lemma makes it coherent and hence dissociated. We prove the remaining case d=q+1d=q+1.

Split O=A⊔BO=A\sqcup B into its two residue classes modulo 2q2q. If one is empty, the same transfer argument, now modulo 2q2q, proves (1). Assume both are nonempty.

Suppose D⊆AD\subseteq A is dissociated and ∣D∣=d|D|=d, and put S=∑DS=\sum D. Every b∈Bb\in B has a ternary representation on DD. If its coefficient sum is ss, reduction modulo 2q2q gives

s≡q+1=d(mod2q),−d≤s≤d.s\equiv q+1=d\pmod{2q},\qquad -d\le s\le d.

The only possibilities are s=ds=d and s=2−ds=2-d. The former representation is all-plus. In the latter, positivity excludes all-negative representations, leaving exactly one positive and d−1d-1 negative coefficients. Thus

b=Sorb=2x−S(x∈D).(2)b=S\quad\hbox{or}\quad b=2x-S\quad(x\in D). \tag{2}

At most one value of the second kind is positive. Consequently, if d(A)=dd(A)=d, then ∣B∣≤2|B|\le2. The same assertion holds with the two fibers interchanged.

If both fibers have at least three elements, they therefore have dimension at most d−1=qd-1=q. Apply the already proved unit-class bound modulo qq to each: their total size is at most 2d−12^{d-1}. It remains to treat a fiber BB of size one or two.

If d(A)≤d−1d(A)\le d-1, then ∣O∣≤2d−2+2≤2d−1|O|\le2^{d-2}+2\le2^{d-1}, so suppose d(A)=dd(A)=d. When B={b,c}B=\{b,c\}, equation (2) shows that every maximum dd-subset of AA contains

x=(b+c)/2.x=(b+c)/2.

Deleting xx lowers the dimension of AA to at most d−1d-1. Applying the unit-class bound to A∖{x}A\setminus\{x\} gives

∣O∣≤2d−2+3≤2d−1,|O|\le2^{d-2}+3\le2^{d-1},

since d≥5d\ge5.

The singleton fiber

Let B={b}B=\{b\}. By a circuit we mean a nonzero ternary relation whose support contains no smaller support of a nonzero ternary relation. Consider all circuits on OO of support size at most d+1d+1.

Every such circuit contained in AA is balanced: its coefficient sum is divisible by 2q2q, and its absolute value is at most d+1=q+2<2qd+1=q+2<2q. A circuit through bb, oriented as b=∑x∈Aεxxb=\sum_{x\in A}\varepsilon_xx, has at most dd other coordinates. The same congruence and positivity argument as in (2) gives exactly two possible forms:

b=∑x∈Ex,∣E∣=d,orb=x−∑y∈E′y,∣E′∣=d−1.(3)b=\sum_{x\in E}x,\quad |E|=d, \qquad\hbox{or}\qquad b=x-\sum_{y\in E'}y,\quad |E'|=d-1. \tag{3}

If b>max⁡Ab>\max A, only the first form is possible. If b<max⁡Ab<\max A, the first form is impossible as well: circuit minimality makes its dd summands dissociated, and adjoining max⁡A>b=∑E\max A>b=\sum E would give a dissociated (d+1)(d+1)-set. Thus all circuits through bb have the same coefficient sum on AA, namely dd when b>max⁡Ab>\max A and 2−d2-d when b<max⁡Ab<\max A.

Let R⊆ZOR\subseteq\mathbb Z^O be generated by the circuits just considered, and put H=ZO/RH=\mathbb Z^O/R. Two integer functionals annihilate RR: the actual weights and the function hh equal to one on AA, with

h(b)=d(b>max⁡A),h(b)=2−d(b<max⁡A).h(b)=d\quad(b>\max A),\qquad h(b)=2-d\quad(b<\max A).

These functionals are rationally independent, since AA contains at least two distinct weights. Hence rank⁡H≥2\operatorname{rank}H\ge2. In particular dim⁡F2(H/2H)≥2\dim_{\mathbb F_2}(H/2H)\ge2.

The actual odd weights give a character λ:H→F2\lambda:H\to\mathbb F_2 equal to one on every coordinate column. Choose a character χ∉{0,λ}\chi\notin\{0,\lambda\}. Its values partition OO into two nonempty classes O0,O1O_0,O_1. Both have dimension at most d−1d-1. For if a dissociated dd-set lay in O0O_0, adjoining a point of O1O_1 would produce a circuit of size at most d+1d+1 using that point; applying χ\chi contradicts that relation. For a dd-set in O1O_1, apply χ+λ\chi+\lambda instead.

The classes are still subsets of the original unit class modulo qq. The established bound at dimension at most q=d−1q=d-1 gives ∣O0∣,∣O1∣≤2d−2|O_0|,|O_1|\le2^{d-2}. This proves (1).

A recursive universal estimate

For d≥1d\ge1 put

Bd=min⁡{2d+⌊log⁡2(d+1)⌋−1−1,2⌈log⁡2d⌉−1(2d−1)},B_d=\min\left\{ 2^{d+\lfloor\log_2(d+1)\rfloor-1}-1, 2^{\lceil\log_2d\rceil-1}(2^d-1) \right\},

where the second term is omitted for d=1d=1. These are the previously proved positive-set bounds: the first follows by applying the binary-tree bound to {0}∪P∪(−P)\{0\}\cup P\cup(-P), and the second is the coherent-support bound.

Set U0=0U_0=0, Ud=2d−1U_d=2^d-1 for 1≤d≤41\le d\le4, and, for d≥5d\ge5,

qd=2⌈log⁡2(d−1)⌉,Ud=min⁡{Bd, qd2d−2+Ud−1}.(4)q_d=2^{\lceil\log_2(d-1)\rceil},\qquad U_d=\min\{B_d,\ q_d2^{d-2}+U_{d-1}\}. \tag{4}

Then every finite positive real set of dimension at most dd has at most UdU_d elements, and every finite real set of dimension at most dd has at most 2Ud+12U_d+1 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 d−1d-1, because one odd element can be adjoined to every dissociated even subset. Partition the odd part into its qd/2q_d/2 unit classes modulo qdq_d. The theorem bounds each by 2d−12^{d-1}, since d≤qd+1d\le q_d+1. This proves the second term of (4), and BdB_d supplies the first. Symmetrization proves the real-set bound.

The first new values are

d56789Ud4712738389519192Ud+19525576717913839.\begin{array}{c|rrrrr} d&5&6&7&8&9\\\hline U_d&47&127&383&895&1919\\ 2U_d+1&95&255&767&1791&3839. \end{array}

In particular every 9696-element real set contains a dissociated six-set. This still does not prove the required six-set for every 6464-element real set. Equivalently, the estimate U5=47U_5=47 does not give the target positive bound U5=31U_5=31.

The remaining unit-congruence gap begins at d=q+2d=q+2. A ternary representation across the two modulo-2q2q 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 4≤d≤q+14\le d\le q+1, to 7 2d−47\,2^{d-4}. Thus (4) can be strengthened: keep U0=0U_0=0 and Ud=2d−1U_d=2^d-1 for 1≤d≤41\le d\le4, and replace its recursion by

Ud=min⁡{Bd, 7qd2d−5+Ud−1}(d≥5).(5)\boxed{U_d=\min\{B_d,\ 7q_d2^{d-5}+U_{d-1}\} \qquad(d\ge5).} \tag{5}

The proof is the same parity split. The first values are now

d56789Ud4312735179916952Ud+18725570315993391.\begin{array}{c|rrrrr} d&5&6&7&8&9\\\hline U_d&43&127&351&799&1695\\ 2U_d+1&87&255&703&1599&3391. \end{array}

In particular every 8888-element real set has a dissociated six-set, but the requested threshold is 6464, still unproved.

The same note proves the unmodified unit-class count through d≤q+2d\le q+2 for even q≥6q\ge6, through d≤q+3d\le q+3 for even q≥10q\ge10, and through d≤⌊4q/3⌋d\le\lfloor4q/3\rfloor for even q≥56q\ge56. 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 q=4,d=6q=4,d=6 was left unresolved by these arguments; it is settled, with bound 3131, by the grid theorem.

Current strengthened recursion

The later fourteen-point theorem gives the affine bound 13 2d−513\,2^{d-5} for d≥5d\ge5. For even q≥6q\ge6 the unit-class argument above propagates that same bound through d=q+1d=q+1: both dropped classes contribute 13 2d−613\,2^{d-6}, and the two-point exception contributes at most 13 2d−6+3≤13 2d−513\,2^{d-6}+3\le13\,2^{d-5}. The already proved case d≤qd\le q follows directly from the affine theorem. The q=4,d=5q=4,d=5 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

(U0,U1,U2,U3,U4,U5,U6)=(0,1,3,6,14,42,104),(U_0,U_1,U_2,U_3,U_4,U_5,U_6)=(0,1,3,6,14,42,104),

and for d≥7d\ge7 set

Ud=min⁡{Bd, 13qd2d−6+Ud−1},qd=2⌈log⁡2(d−1)⌉.(6)\boxed{U_d=\min\{B_d,\ 13q_d2^{d-6}+U_{d-1}\}, \qquad q_d=2^{\lceil\log_2(d-1)\rceil}.} \tag{6}

Then ∣P∣≤Ud(P)|P|\le U_{d(P)} for positive sets, and ∣A∣≤2Ud(A)+1|A|\le2U_{d(A)}+1 for arbitrary real sets.

For the new starting values, the established odd bounds through dimension four are 1,2,4,81,2,4,8. The sharp positive bound U3=6U_3=6 therefore gives U4=8+6=14U_4=8+6=14. Splitting an odd dimension-five set modulo four gives at most 2828 elements, hence U5=28+14=42U_5=28+14=42. The grid theorem bounds each modulo-four class of a dimension-six odd set by 3131, so its size is at most 6262 and U6=62+42=104U_6=62+42=104. Each use of the even-part bound is justified by adjoining an odd element after normalization. For d≥7d\ge7, there are qd/2q_d/2 odd classes, each bounded by 13 2d−513\,2^{d-5}, proving (6).

In particular,

d3456789Ud6144210431272815602Ud+113298520962514573121.\begin{array}{c|rrrrrrr} d&3&4&5&6&7&8&9\\\hline U_d&6&14&42&104&312&728&1560\\ 2U_d+1&13&29&85&209&625&1457&3121. \end{array}

Thus every 8686-element real set has a dissociated six-set, and every 210210-element real set has a dissociated seven-set. The required thresholds 6464 and 128128 remain unproved.