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Coefficient-safe profile compression of root colorings


Result and exact limitation

This is a new necessary condition on a putative proper finite coloring of the prime tensor family, not a proof that such a coloring is impossible. It uses the full signed relation system and makes no Galois-equivariance assumption.

Let ff be a proper qq-coloring of the squarefree odd-root grid, viewed as the set of finite-support tuples in ∏p≥3[p]\prod_{p\geq3}[p] after fixing a basepoint in each prime coordinate. Declare two symbols in coordinate pp equivalent when replacing one by the other leaves the color unchanged for every finite-support assignment of all other coordinates. Let mpm_p be the number of these coordinate profiles. Then

mp≥2,∑p≥3(1mp−1p)≤2log⁡(48q)<∞.(1)m_p\geq2,\qquad \sum_{p\geq3}\left(\frac1{m_p}-\frac1p\right) \leq2\log(48q)<\infty. \tag{1}

In particular, for every fixed 0<ε<10<\varepsilon<1,

∑p:mp≤(1−ε)p1p<∞.(2)\sum_{p:m_p\leq(1-\varepsilon)p}\frac1p<\infty. \tag{2}

The same quantitative bound holds at each sufficiently long finite prime prefix, using profiles of that finite coloring. The equivalence classes may change with the prefix; no compatibility between finite colorings is needed.

More precisely, the finite assertion applies to all odd primes through P≥e5P\geq e^5, with counts mp,Pm_{p,P} taken from that finite coloring. It bounds ∑p≤P(1/mp,P−1/p)\sum_{p\leq P}(1/m_{p,P}-1/p) but does not assert monotonicity as PP varies. For a single global coloring, its global profile classes are valid compression blocks on each finite prefix, although the restricted profiles may merge some of them. Apply the finite compression lemma to those global blocks themselves; only their partial deficit sums are then passed monotonically to the infinite sum in (1).

An arbitrary finite coloring can have mp=pm_p=p everywhere. We have not proved that properness prevents this, or otherwise forces a violation of (1). Thus the unrestricted coloring theorem in the main argument remains unproved.

1. A finite compression lemma

Let E=⨂i=1kSpiE=\bigotimes_{i=1}^k S_{p_i}, with simplex columns si,1,…,si,pis_{i,1},\ldots,s_{i,p_i}. Partition the symbols in each coordinate into nonempty blocks Ai,1,…,Ai,miA_{i,1},\ldots,A_{i,m_i}. Assume the color is unchanged by replacing a symbol inside one block, with all other coordinates arbitrary. Equivalently it is constant on every product box of these blocks.

If mi=1m_i=1, any full coordinate-ii fiber is monochromatic and its columns sum to zero, contradicting properness. Suppose therefore all mi≥2m_i\geq2, and put

wi,a=∑x∈Ai,asi,x.w_{i,a}=\sum_{x\in A_{i,a}}s_{i,x}.

These vectors have precisely the one rational relation ∑awi,a=0\sum_a w_{i,a}=0. Indeed a dependence with coefficients tat_a expands to a simplex dependence whose coefficient on each symbol in Ai,aA_{i,a} is tat_a; the simplex kernel consists exactly of constant coefficient vectors. Hence all tat_a must be equal. The vectors are therefore a linear copy of SmiS_{m_i}.

Color the indexed compressed tensor ⨂iSmi\bigotimes_i S_{m_i} by the common color of each corresponding box. Suppose a same-colored collection of its indexed columns had a nonzero signed relation. Expanding each column ⨂iwi,ai\bigotimes_iw_{i,a_i} sums the original columns in its box. Distinct boxes are disjoint. Every expanded coefficient remains 00 or ±1\pm1, and at least one coefficient is nonzero. This is a monochromatic signed relation in EE, impossible.

Thus the induced compressed coloring is proper. Retaining the indices matters when mi=2m_i=2: antipodal factors can produce repeated tensor values, and relations between their distinct labels must not be discarded.

2. Quantitative restriction on the compressed sides

For any indexed tensor with sides mi≥2m_i\geq2, set

N=∏imi,d=∏i(mi−1),R=d/N,L=∑ilog⁡(mi−1)mi.N=\prod_i m_i,\qquad d=\prod_i(m_i-1),\qquad R=d/N,\qquad L=\sum_i\frac{\log(m_i-1)}{m_i}.

A proper qq-coloring necessarily satisfies

1q<4R(1+2Llog⁡2).(3)\frac1q<4R\left(1+\frac{2L}{\log2}\right). \tag{3}

This is the small-column entropy bound, whose proof also works for indexed sides of size two. Here are the needed details. In standard integer coordinates the average log column ℓ1\ell_1-norm is LL. At least N/2N/2 labels have column norm at most e2Le^{2L} (if L=0L=0, all do). Some color contains at least N/(2q)N/(2q) of these labels. If ss of them are dissociated, their subset sums are distinct and have total coordinate-box width at most se2Ls e^{2L}. Hence

2s≤(1+se2L/d)d.2^s\leq(1+s e^{2L}/d)^d.

The elementary implication 2t≤1+Mt⇒t<2log⁡2(2M)2^t\leq1+Mt\Rightarrow t<2\log_2(2M), for M≥1M\geq1, gives s<2d(1+2L/log⁡2)s<2d(1+2L/\log2). Combining the lower and upper bounds proves (3).

For example, if 2≤mi≤M2\leq m_i\leq M uniformly, (3) implies

q>(M/(M−1))k4(1+klog⁡(M−1)/log⁡2).(4)q> \frac{(M/(M-1))^k} {4\bigl(1+k\log(M-1)/\log2\bigr)}. \tag{4}

Thus bounded coordinate-profile counts cannot properly color arbitrarily many tensor factors with a fixed palette. More generally every schedule with Rk(1+Lk)→0R_k(1+L_k)\to0 is excluded.

3. The summable prime-profile deficit

Use all odd prime coordinates p≤Pp\leq P, and define

D=D(P)=∑3≤p≤P(1mp−1p)≥0.D=D(P)=\sum_{3\leq p\leq P}\left(\frac1{m_p}-\frac1p\right)\geq0.

The elementary Euler product gives

∏p≤P(1−1/p)−1≥∑n≤⌊P⌋1n≥log⁡P.\prod_{p\leq P}(1-1/p)^{-1} \geq\sum_{n\leq\lfloor P\rfloor}\frac1n\geq\log P.

Indeed every integer n≤Pn\leq P has all its prime factors at most PP, and H⌊P⌋≥log⁡(⌊P⌋+1)≥log⁡PH_{\lfloor P\rfloor}\geq\log(\lfloor P\rfloor+1)\geq\log P. For m≤pm\leq p, log⁡(1−1/m)−log⁡(1−1/p)≤−(1/m−1/p)\log(1-1/m)-\log(1-1/p)\leq-(1/m-1/p). Removing the prime two from the Euler product therefore gives

R≤2e−Dlog⁡P.(5)R\leq\frac{2e^{-D}}{\log P}. \tag{5}

The proved elementary prime estimate ∑p≤P(log⁡p)/p≤log⁡P+5\sum_{p\leq P}(\log p)/p\leq\log P+5 also gives

L≤∑3≤p≤Plog⁡pmp≤log⁡P+5+Dlog⁡P.(6)\begin{aligned} L&\leq\sum_{3\leq p\leq P}\frac{\log p}{m_p}\\ &\leq\log P+5+D\log P. \end{aligned} \tag{6}

No lower bound on mp/pm_p/p is assumed here. For P≥e5P\geq e^5, substitution in (3) yields

1q<8e−D[1log⁡P+2log⁡2(1+D+5log⁡P)]<24(D+2)e−D≤48e−D/2.(7)\frac1q<8e^{-D} \left[\frac1{\log P}+\frac2{\log2} \left(1+D+\frac5{\log P}\right)\right] <24(D+2)e^{-D}\leq48e^{-D/2}. \tag{7}

For the middle estimate one may use 2/log⁡2<2.92/\log2<2.9; the bracket is at most 0.2+2.9(D+2)≤3(D+2)0.2+2.9(D+2)\leq3(D+2), with strictness from the logarithmic bound. The last estimate follows from D+2≤2eD/2D+2\leq2e^{D/2}. Thus D(P)<2log⁡(48q)D(P)<2\log(48q). For a global coloring its partial deficit sums increase, proving (1). Equation (2) follows because each summand at such a prime is at least ε/[(1−ε)p]\varepsilon/[(1-\varepsilon)p].

4. A rigorously excluded algorithmic class

A deterministic fixed-order finite-state scan with at most ss states has at most sss^s coordinate profiles. Precisely, its successive updates are δi:Qi−1×[pi]→Qi\delta_i:Q_{i-1}\times[p_i]\to Q_i, with ∣Qi∣≤s|Q_i|\leq s, and its output is determined by the final state. Each input symbol induces one of at most sss^s maps Qi−1→QiQ_{i-1}\to Q_i. Symbols with the same map are interchangeable in every prefix/suffix context. This applies even when the fixed reading order and transition maps vary with the prime or the finite grid size.

With M=ssM=s^s, (4) rules out fixed-palette, bounded-state read-once colorings for arbitrarily many factors. A one-state procedure is already constant and fails on a simplex fiber. This theorem does not cover adaptive reading orders, arbitrary algorithms, growing state spaces, or unrestricted mathematical colorings.

The useful new mechanism is coefficient-safe block-sum compression. The unsolved next step would require an additional argument from dissociation itself, not merely from the finiteness of the palette, to produce enough compression or another forbidden signed relation.

Exact scope

The compression hypothesis is exact monochromaticity of every product box; agreement in only selected contexts or approximate agreement does not suffice. The prime-deficit constant uses the complete odd-prime prefix and is not asserted unchanged for an arbitrary sparse prime family. The finite-state consequence assumes the fixed-order scan model stated above. Most importantly, the theorem does not rule out the all-distinct-profile case mp=pm_p=p, and no proper coloring realizing that case has been constructed here either.