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Fixed-height chromatic growth suffices for full dissociation


Standing

The piecewise-syndetic reformulation is equivalent to the fixed-height premise below. That page also constructs an ordinary idempotent containing a dissociated root set, with infinite rational coloring number in every member. Thus rational dependence in all members, even with idempotence, does not replace one common finite height.

This is a positive, elementary focusing reduction for the exact gap in the main argument. It does not establish its hypothesis. Unlike a bare monochromatic-rectangle assertion, it explicitly pays for the whole-profile palette and for every excluded conductor prime.

Let

G=⨁p odd primeμpG=\bigoplus_{p\text{ odd prime}}\mu_p

be the multiplicative group of odd squarefree-order complex roots. Additive relations always refer to their values in C\mathbb C. For h≥1h\geq1, write χh(X)\chi_h(X) for the least number of classes with no nonzero integer relation having every coefficient in [−h,h][-h,h]. Thus χ1\chi_1 is the dissociated coloring number. This is a bound on coefficient magnitude, not the fixed-order notion of hh-freeness of Nešetřil–Rödl–Sales.

Theorem

If χh(G)=∞\chi_h(G)=\infty for one fixed finite hh, then χ1(G)=∞\chi_1(G)=\infty. Consequently

χ1(G)<∞⟺χh(G)<∞ for every finite h.(1)\chi_1(G)<\infty \quad\Longleftrightarrow\quad \chi_h(G)<\infty\text{ for every finite }h. \tag{1}

The forward implication is special to this multiplicatively closed root family and the focusing argument below; it is not asserted for arbitrary integer sets. In fact, for each fixed finite hh, finiteness of χ1(G)\chi_1(G) and of χh(G)\chi_h(G) are equivalent.

Finite witnesses and conductor tails

For a finite set SS of odd primes, put TS=⨁p∉S, p oddμpT_S=\bigoplus_{p\notin S,\ p\text{ odd}}\mu_p. If TST_S had a finite hh-independent coloring, using separate palettes on its finitely many multiplicative cosets would color GG: multiplication by a nonzero root preserves every integer relation. Therefore

χh(G)=∞⟹χh(TS)=∞for every finite S.(2)\chi_h(G)=\infty\quad\Longrightarrow\quad \chi_h(T_S)=\infty\quad\text{for every finite }S. \tag{2}

An infinite chromatic number has finite witnesses. Indeed, if every finite subset of a countable set had a proper qq-coloring, take colorings of nested finite exhaustions and successively stabilize each vertex color along infinite subsequences. The resulting coloring avoids every forbidden relation, because its support is finite. Apply the contrapositive for each qq.

Focusing induction with a fixed height

Assume χh(G)=∞\chi_h(G)=\infty. We prove the following statement simultaneously for every finite SS, every palette size qq, and every r≥1r\geq1:

Every qq-coloring of TST_S contains finite height-hh dependent sets X1,…,XrX_1,\ldots,X_r in pairwise coprime conductor groups, disjoint from SS, whose full product X1⋯XrX_1\cdots X_r is monochromatic.

For r=1r=1, use (2). Suppose the statement holds for r−1r-1, with all finite palettes. Choose a finite F⊂TSF\subset T_S with χh(F)>q\chi_h(F)>q, and let JJ be its conductor-prime set. Given f:TS→[q]f:T_S\to[q], color TS∪JT_{S\cup J} by the complete finite profiles

y⟼(f(xy))x∈F∈[q]F.y\longmapsto (f(xy))_{x\in F}\in[q]^F.

There are at most q∣F∣q^{|F|} profile colors. The induction hypothesis at that palette supplies r−1r-1 conductor-disjoint height-hh dependent sets whose product YY has one profile g:F→[q]g:F\to[q]. Since χh(F)>q\chi_h(F)>q, one color class of gg contains a nonzero height-hh relation. Take its support as X1X_1. Then f(xy)f(xy) is one fixed color for every x∈X1x\in X_1, y∈Yy\in Y. The conductors of X1X_1 and all the other factors are coprime by construction. This completes the induction without any bound on ∣F∣|F| or the profile palette: the hypothesis permits every finite palette at the same height.

For h≥2h\geq2, take r=hr=h and apply the proved Hall/determinant flattening lemma. It gives a nonzero monochromatic ternary relation. This holds for every qq, so χ1(G)=∞\chi_1(G)=\infty. The case h=1h=1 is immediate. Finally χh≥χ1\chi_h\geq\chi_1, proving the other direction of (1).

Exact unresolved quantifier

The previously proved bounded-height result has the form

∀q ∃h=h(q)χh(G)>q,h(q)=⌈e3q⌉ is sufficient.(3)\forall q\ \exists h=h(q)\quad \chi_h(G)>q, \qquad h(q)=\lceil e^{3q}\rceil\text{ is sufficient}. \tag{3}

The focusing theorem instead needs

∃h<∞ ∀qχh(G)>q.(4)\exists h<\infty\ \forall q\quad\chi_h(G)>q. \tag{4}

There is no exchange of these quantifiers. Finite numbers χh(G)\chi_h(G) growing with hh satisfy (3) without satisfying (4). In particular, applying (3) at q∣F∣q^{|F|} changes the height and invalidates the fixed-height induction.

A proof of (4), even for h=2h=2, would be a genuine route to completing the required counterexample: the theorem gives unbounded ternary coloring on finite odd-prime grids, and the already proved uniform extraction, exact integer encoding, and separated-block assembly then apply. No such fixed height is currently known in this package.

Finite quantitative formulation

If finite conductor-disjoint factors FiF_i, ni=∣Fi∣n_i=|F_i|, satisfy

χh(Fi)>q n1⋯ni−1,(5)\chi_h(F_i)>q^{\,n_1\cdots n_{i-1}}, \tag{5}

with empty product one, every qq-coloring of their product has a monochromatic product of height-hh dependent subsets. Start with the last factor, color it by all prefix profiles, and select a dependent profile class. The common profile is a coloring of the shorter prefix; repeat. For hh factors, determinant flattening applies.

Conditionally on χh(G)=∞\chi_h(G)=\infty, put κh(t)=min⁡{k:χh(Ek)>t}\kappa_h(t)=\min\{k:\chi_h(E_k)>t\}, and let Nk=∣Ek∣N_k=|E_k|. Define k0=0k_0=0, N0=1N_0=1, and

ki=κh(Nki−1qNki−1).k_i=\kappa_h\bigl(N_{k_{i-1}}q^{N_{k_{i-1}}}\bigr).

These indices increase: χh(Ek)≤Nk\chi_h(E_k)\leq N_k excludes earlier ones. The consecutive prime blocks FiF_i satisfy (5), since coloring their Nki−1N_{k_{i-1}} prefix slices separately gives χh(Eki)≤Nki−1χh(Fi)\chi_h(E_{k_i})\leq N_{k_{i-1}}\chi_h(F_i). Thus χ1(Ekh)>q\chi_1(E_{k_h})>q. This is a bound in terms of an unproved finite witness function, not a new numerical chromatic estimate.

A conditional idempotent formulation

This formulation records a second rigorous focusing mechanism; no existence or minimality theorem for ultrafilters is used. Let U\mathcal U be an ultrafilter on GG, with RB={x:x−1B∈U}R_B=\{x:x^{-1}B\in\mathcal U\}, and suppose it is idempotent, meaning B∈UB\in\mathcal U if and only if RB∈UR_B\in\mathcal U.

Proposition. If one finite hh works so that every member of U\mathcal U contains a height-hh dependence, every member contains a ternary dependence. Consequently, if U\mathcal U contains a dissociated set, it contains nested hh-independent sets for all finite hh.

For A∈UA\in\mathcal U, set A∗=A∩RAA^*=A\cap R_A. It belongs to U\mathcal U; for x∈A∗x\in A^*, both x−1Ax^{-1}A and x−1RA=Rx−1Ax^{-1}R_A=R_{x^{-1}A} belong to U\mathcal U, so x−1A∗∈Ux^{-1}A^*\in\mathcal U. Every finite-prime tail TST_S also belongs to U\mathcal U: the ultrafilter selects a coset aTSaT_S in the finite quotient, and RaTS=TSR_{aT_S}=T_S; apply idempotence.

Construct hh factors inductively. If PP is the finite set of all nonempty products taking at most one point from the preceding factors, and SS contains their conductor primes, choose the next dependent support in

TS∩A∗∩⋂s∈Ps−1A∗∈U.T_S\cap A^*\cap\bigcap_{s\in P}s^{-1}A^*\in\mathcal U.

The invariant P⊂A∗P\subset A^* persists. All conductors are disjoint, and the full product lies in A∗A^*. Determinant flattening proves the proposition. Its contrapositive supplies an hh-independent member for each hh; intersect these successively with the dissociated member to make them nested.

For h=1h=1, the proposition is immediate from its hypothesis; the determinant step is needed only for h≥2h\geq2.

Covering information does not supply uniform height

Call FBFB thick if, for every finite E⊂GE\subset G, some translate tEtE is contained in FBFB. If this holds with finite FF, k=∣F∣k=|F|, and BB is hh-independent, assigning each x∈Ex\in E an f∈Ff\in F with f−1tx∈Bf^{-1}tx\in B properly hh-colors EE with kk colors. The existing small-column inequality, on all odd-prime prefixes and with P→∞P\to\infty, gives

log⁡(h+1)≤2k.\log(h+1)\leq2k.

The explicit earlier height ⌈e3k⌉\lceil e^{3k}\rceil therefore forces a dependence in a set with such a kk-element thick-cover witness.

But these cover sizes cannot be uniformly bounded inside an idempotent ultrafilter, even after fixing one member AA. For finite SS, A∩TS∈UA\cap T_S\in\mathcal U, and any finite FF with F(A∩TS)F(A\cap T_S) thick has

∣F∣≥[G:TS]=∏p∈Sp.|F|\geq[G:T_S]=\prod_{p\in S}p.

A thick set projects onto the entire finite quotient, while the displayed product projects into the image of FF. This only disproves a uniform bound on these covering witnesses; it does not independently prove that minimal relation heights grow. The missing exchange is still from member-dependent heights to one height for every member.

The elementary finite focusing theorem and its finite quantitative form received an independent internal audit. All new proofs here are algebraic or finite-color compactness arguments, with no numerical experiment.