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High-girth counting and algebraic obstructions


These are partial results. They do not settle the regime with many short ternary relations left open in the proof sketch.

A proved counting inequality

Let PP be a nonempty finite positive real set, let n=∣P∣n=|P|, and let d=d(P)d=d(P). Let gg be the minimum support size of a nonzero ternary relation on PP, with g=∞g=\infty if PP is dissociated. For every positive integer h≤nh\le n with 2h<g2h<g,

(nh)≤(2h+1)d−12.(1)\binom nh\le\frac{(2h+1)^d-1}{2}. \tag{1}

Indeed, choose a maximum dissociated D⊆PD\subseteq P. Maximality represents every element of PP as a ternary combination of DD. Every sum of an hh-element subset of PP is therefore an image of an integer vector in [−h,h]d[-h,h]^d. Distinct such subsets have distinct sums: otherwise canceling their intersection gives a nonzero ternary relation of support at most 2h2h. All their sums are positive. The nonzero vectors of the cube occur in opposite pairs, each of which contributes at most one positive image. There are ((2h+1)d−1)/2((2h+1)^d-1)/2 such pairs. This argument does not require rational independence of DD.

Consequently, a counterexample n≥2dn\ge2^d with d≥9d\ge9 must have a ternary relation of support at most six. Otherwise (1), with h=3h=3, contradicts

(5123)=22 238 720>79−12=20 176 803.\binom{512}{3}=22\,238\,720> \frac{7^9-1}{2}=20\,176\,803.

The contradiction persists as dd increases: the ratio (2N3)/(N3)\binom{2N}{3}/\binom N3 is greater than 88, whereas (7d+1−1)/(7d−1)=7+6/(7d−1)<8(7^{d+1}-1)/(7^d-1)=7+6/(7^d-1)<8 for d≥2d\ge2.

Also, the target n≤2d−1n\le2^d-1 holds whenever g≥9g\ge9. If PP were a counterexample, maximality of DD would give g≤d+1g\le d+1, so d≥8d\ge8. But the h=4h=4 case of (1) excludes a counterexample already for every d≥5d\ge5:

(324)=35 960>95−12=29 524.\binom{32}{4}=35\,960>\frac{9^5-1}{2}=29\,524.

Under doubling of NN, the left-hand side grows by a factor greater than 1616; the ratio on the right is 9+8/(9d−1)<169+8/(9^d-1)<16. The already dissociated case is immediate.

A domain alone does not give the required product-space principle

For elements f1,…,fkf_1,\ldots,f_k of a field extension, call their squarefree products independent if the 2k2^k products ∏i∈Ifi\prod_{i\in I}f_i are linearly independent over the base field. There is no bound of the desired type using only the dimension of span⁡{1,f1,…,fn}\operatorname{span}\{1,f_1,\ldots,f_n\} in a domain.

For distinct rational numbers aia_i, put fi=1/(t−ai)∈Q(t)f_i=1/(t-a_i)\in\mathbb Q(t). The functions 1,f1,…,fn1,f_1,\ldots,f_n are linearly independent, as their distinct simple poles show. However,

fifj=fi−fjai−aj(i≠j).f_i f_j=\frac{f_i-f_j}{a_i-a_j}\qquad(i\ne j).

Thus the largest subset with independent squarefree products has size one, for arbitrarily large nn. A linear-product argument must use the distinguished monomial basis of a group algebra, not just the absence of zero divisors.

Generic linear combinations cannot simply be extracted to monomials

Even inside a monomial space, independent squarefree products of linear combinations need not yield a monomial subset of the same size. The exponent set {1,2,3}\{1,2,3\} has dissociation dimension two. But in W=span⁡Q{x,x2,x3}W=\operatorname{span}_{\mathbb Q}\{x,x^2,x^3\}, the three elements

f1=x+x2,f2=x2+x3,f3=x+x3f_1=x+x^2,\qquad f_2=x^2+x^3,\qquad f_3=x+x^3

have all eight squarefree products linearly independent.

The three single factors are independent in degrees one through three: their coefficient determinant is 22. The coefficient matrix of f1f2,f1f3,f2f3f_1f_2,f_1f_3,f_2f_3 in degrees four through six is

(210110111),\begin{pmatrix}2&1&0\\1&1&0\\1&1&1\end{pmatrix},

whose determinant is 11. Hence their classes are independent modulo the span of the constant and the single factors. Finally, the triple product has degree eight, greater than every pair product. These facts prove independence of all eight products. Any extraction from generic linear combinations therefore needs an additional argument not supplied by determinant expansion alone.

The extraction obstruction also works in characteristic two

The determinant 22 in the preceding example does not make characteristic two an exception. Over any field, take

f1=t2,f2=t3,f3=t+t2+t3f_1=t^2,\qquad f_2=t^3,\qquad f_3=t+t^2+t^3

in the monomial space on exponents {1,2,3}\{1,2,3\}. Their singles span t,t2,t3t,t^2,t^3. Their pair products are

t5,t3+t4+t5,t4+t5+t6.t^5,\qquad t^3+t^4+t^5,\qquad t^4+t^5+t^6.

Modulo the span of 1,t,t2,t31,t,t^2,t^3, their coefficient matrix in degrees four, five, and six has determinant −1-1. The triple product t6+t7+t8t^6+t^7+t^8 adds degree eight. Thus all eight squarefree products are independent over any field, although the exponent set has dissociation dimension two. Passing to a group algebra of characteristic two does not repair generic-linear-combination extraction.

A simple binary-matroid replacement is impossible

One proposed weaker alternative to a cube-spanned lift was a simple binary matroid on PP such that every matroid-independent subset is arithmetically dissociated. Its rank would be at most d(P)d(P), and simplicity would give the desired cardinality bound. Such a replacement does not always exist, in any rank.

Take P={1,2,3,4}P=\{1,2,3,4\}. In a simple binary representation, all column vectors v1,v2,v3,v4v_1,v_2,v_3,v_4 are distinct and nonzero, so every pair is independent. The arithmetic dependencies 1+2=31+2=3 and 1+3=41+3=4 would require both corresponding triples to be dependent in the binary matroid. Therefore

v1+v2+v3=0,v1+v3+v4=0,v_1+v_2+v_3=0,\qquad v_1+v_3+v_4=0,

giving v2=v4v_2=v_4, a contradiction.

This excludes that binary-matroid model, not the cubical covering statement: the latter does not require arithmetic circuits to become binary-matroid dependencies.