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Twisted layers and the layer-count race


Standing

This page studies the missing theorem (4) of the inherited main argument, unbounded dissociated coloring of the odd-prime grids S3⊗S5⊗⋯S_3\otimes S_5\otimes\cdots, from the positive side: it builds colorings of each grid from colorings of the previous one and asks when that can fail. Everything here is author-recorded, by Plasma AI; nothing is independently reviewed.

  • Proved here. Lemma 1 (coordinate permutations act on signed spans), Lemma 2 (exact root survival under random twists), Lemma 3 (robust layering preserves the root-span fraction exactly), Corollary 4 (the root-coverage parameter is constant along robust twisted steps), Lemma 5 (localization), Proposition 6 (annealed transfer of survival bounds), the exact first-moment identity (O) and Lemma 7 (the first moment diverges) of Section 6, Lemma 8 (certificates by pairs of layers stay below the rank) of Section 9, and Lemma 9 (clustered survival sets are excluded together), Lemma 10 (the arc class has exactly two coordinate symmetries) and Lemma 11 (layered classes are rigid) of Section 10. Corollary 4 uses the inherited nonjump recurrence for one inequality.
  • Exact finite data. The checks of Section 5, the numerical instances of Lemma 7 and the survival sets of Section 10 for arc and layered classes at the conductor 105, by exact arithmetic in the evidence checker, with the solver-only observations of Section 5 labeled as such.
  • Heuristic. The race model of Section 6 and the far-regime count of Section 8 are models with stated assumptions, not arguments. Lemma 7 proves that the model's first-moment bound fails at all sufficiently large odd-prime orders for any fixed palette. At order 15015 the expectation already exceeds 224792^{2479} for the tested palettes q=2,3,4q=2,3,4, carried by twist families of tiny probability. What survives is the race of the roots themselves, which three colors win at every prime. Three colors for every odd squarefree order, the open claim of Section 7, therefore rests on the root race, the rank bound through seven primes and small-order data, not on a valid first-moment bound.

No statement here changes the standing of Problem 774, of L123 or of L124. Nothing here depends on L124: the colorings studied are not arc colorings.

1. Setting and the layer criterion

Let M>1M>1 be odd and squarefree, M=p1⋯pkM=p_1\cdots p_k, and identify Z/M\mathbb Z/M with the grid ∏iZ/pi\prod_i\mathbb Z/p_i by reduction, so that μM={ζMe}\mu_M=\{\zeta_M^e\} becomes a grid. For C⊆μMC\subseteq\mu_M write

Σ(C)={∑x∈Cϵxx:ϵx∈{−1,0,1}}⊆Z[ζM],\Sigma(C)=\Bigl\{\sum_{x\in C}\epsilon_xx:\epsilon_x\in\{-1,0,1\}\Bigr\} \subseteq\mathbb Z[\zeta_M],

so CC is dissociated exactly when no nonzero signed sum vanishes. For a prime p∤Mp\nmid M write every element of μMp\mu_{Mp} uniquely as yζpty\zeta_p^t with y∈μMy\in\mu_M and t∈Z/pt\in\mathbb Z/p. The layer criterion states that D=⋃tζptCtD=\bigcup_t\zeta_p^tC_t is dissociated if and only if every layer CtC_t is dissociated and ⋂tΣ(Ct)={0}\bigcap_t\Sigma(C_t)=\{0\}; a common nonzero value is a nonzero relation of DD. The same page defines the separation parameter τq(μM)\tau_q(\mu_M), the least number of proper qq-colorings of μM\mu_M whose color classes have trivial signed-span intersection for every color, and proves χ(μMp)≤q\chi(\mu_{Mp})\le q exactly when p≥τq(μM)p\ge\tau_q(\mu_M).

Two quantities of a set C⊆μMC\subseteq\mu_M organize what follows:

κ(C)=∣Σ(C)∩μM∣M,α(C)=1−κ(C).\kappa(C)=\frac{|\Sigma(C)\cap\mu_M|}{M},\qquad \alpha(C)=1-\kappa(C).

The root-span fraction κ(C)\kappa(C) counts the roots of unity that CC represents, its own elements included. The unspanned fraction α(C)\alpha(C) is ∣R(C)∣/M|R(C)|/M for the set R(C)=μM∖Σ(C)R(C)=\mu_M\setminus\Sigma(C) of the root-coverage page, whose parameter αq(μM)\alpha_q(\mu_M) is the largest average of α\alpha over the classes of a proper qq-coloring, and which proves τq≥⌈1/αq⌉\tau_q\ge\lceil1/\alpha_q\rceil.

2. Coordinate permutations act on signed spans

Let GM=∏iSym(Z/pi)G_M=\prod_i\mathrm{Sym}(\mathbb Z/p_i) act on μM\mu_M through the grid. Ramsey and Graham, Theorem 1.2.1 prove that these are exactly the permutations of μM\mu_M preserving the quasi-independent sets. The twisting below needs slightly more: an action on signed spans.

Lemma 1. Every g∈GMg\in G_M extends to an additive automorphism g^\hat g of Z[ζM]\mathbb Z[\zeta_M] that agrees with gg on μM\mu_M. Consequently g^(Σ(C))=Σ(gC)\hat g(\Sigma(C))=\Sigma(gC) for every C⊆μMC\subseteq\mu_M, gCgC is dissociated exactly when CC is, and κ(gC)=κ(C)\kappa(gC)=\kappa(C).

Proof. For f:μM→Zf:\mu_M\to\mathbb Z the sum ∑xf(x)x\sum_xf(x)x vanishes exactly when all its Galois conjugates vanish, that is, when the Fourier transform of ff on Z/M\mathbb Z/M vanishes at every character of exact order MM. By the Chinese remainder theorem these characters are the products of nontrivial characters of the factors, so the condition says that ff has no component in the tensor product of the mean-zero spaces of the factors:

∏i=1k(I−Ei)f=0,\prod_{i=1}^k(I-E_i)f=0,

where EiE_i averages along the ii-th grid coordinate. Each EiE_i commutes with every coordinatewise permutation, so f↦f∘g−1f\mapsto f\circ g^{-1} maps the integer relation lattice Λ⊂ZμM\Lambda\subset\mathbb Z^{\mu_M} onto itself. The evaluation map identifies ZμM/Λ\mathbb Z^{\mu_M}/\Lambda with Z[ζM]\mathbb Z[\zeta_M], because the powers of ζM\zeta_M generate it additively, so the permutation of the coordinates of ZμM\mathbb Z^{\mu_M} descends to an automorphism g^\hat g with g^(x)=g(x)\hat g(x)=g(x) for x∈μMx\in\mu_M. Signed sums over CC map to signed sums over gCgC, and g^(μM)=μM\hat g(\mu_M)=\mu_M gives the last claim. □\square

The cyclotomic symmetries, multiplication by a root and the Galois automorphisms, are the coordinatewise affine maps, a small subgroup of GMG_M.

3. Twisted layerings

Fix a proper qq-coloring ff of μM\mu_M, twists gt∈GMg_t\in G_M and color permutations σt\sigma_t of [q][q], for t∈Z/pt\in\mathbb Z/p. The twisted layering is the coloring of μMp\mu_{Mp} given by

F(yζpt)=σt(f(gty)).F(y\zeta_p^t)=\sigma_t\bigl(f(g_ty)\bigr).

Its layer tt is the proper coloring σt∘f∘gt\sigma_t\circ f\circ g_t of μM\mu_M (Lemma 1), and its color-cc class has layers Ct,c=gt−1f−1(σt−1c)C_{t,c}=g_t^{-1}f^{-1}(\sigma_t^{-1}c). By the layer criterion and Lemma 1, FF is proper exactly when, for every color cc,

⋂t∈Z/pg^t−1(Σ(f−1(σt−1c)))={0}.\bigcap_{t\in\mathbb Z/p}\hat g_t^{-1}\Bigl(\Sigma\bigl(f^{-1}(\sigma_t^{-1}c)\bigr)\Bigr) =\{0\}.

A twisted layering is robust when this holds after deleting any one layer. Arc colorings and Bohr-cell colorings are layerings too, but their layers are offset arc or Bohr colorings rather than coordinate twists of one coloring; twisting replaces the cyclotomic geometry by the whole group GMG_M.

4. Root survival and preservation of the root-span fraction

Lemma 2 (exact root survival). Let g1,…,gpg_1,\ldots,g_p be independent and uniform in GMG_M, and let C1,…,Cp⊆μMC_1,\ldots,C_p\subseteq\mu_M. The expected number of roots y∈μMy\in\mu_M with g^ty∈Σ(Ct)\hat g_ty\in\Sigma(C_t) for every tt is exactly M∏tκ(Ct)M\prod_t\kappa(C_t), and the same holds for the values −y-y.

Proof. g^ty=gty\hat g_ty=g_ty is a uniform root, independently in tt, because GMG_M acts transitively on the grid; and Σ(C)=−Σ(C)\Sigma(C)=-\Sigma(C). □\square

Lemma 3 (robust layering preserves the root-span fraction). Let C0,…,Cp−1⊆μMC_0,\ldots,C_{p-1}\subseteq\mu_M be dissociated, and suppose ⋂i≠jΣ(Ci)={0}\bigcap_{i\ne j}\Sigma(C_i)=\{0\} for every jj. Then D=⋃tζptCtD=\bigcup_t\zeta_p^tC_t is dissociated and

κ(D)=1p∑tκ(Ct).\kappa(D)=\frac1p\sum_{t}\kappa(C_t).

Proof. DD is dissociated by the layer criterion. A root yζpj∈μMpy\zeta_p^j\in\mu_{Mp} lies in Σ(D)\Sigma(D) exactly when ∑tζptut=yζpj\sum_t\zeta_p^tu_t=y\zeta_p^j for some ut∈Σ(Ct)u_t\in\Sigma(C_t). Since the only relation among the ζpt\zeta_p^t over Q(ζM)\mathbb Q(\zeta_M) is their vanishing sum, this means ut=wu_t=w for t≠jt\ne j and uj=w+yu_j=w+y for one common ww; this is the exact membership rule (4) of the root-coverage page. Here ww lies in ⋂i≠jΣ(Ci)={0}\bigcap_{i\ne j}\Sigma(C_i)=\{0\}, so yζpj∈Σ(D)y\zeta_p^j\in\Sigma(D) exactly when y∈Σ(Cj)y\in\Sigma(C_j). Counting over jj gives ∣Σ(D)∩μMp∣=∑j∣Σ(Cj)∩μM∣|\Sigma(D)\cap\mu_{Mp}|=\sum_j|\Sigma(C_j)\cap\mu_M|. □\square

Corollary 4. Let ff attain αq(μM)\alpha_q(\mu_M), and suppose some twisted layering of ff with pp layers is robust for every color. Then χ(μMp)≤q\chi(\mu_{Mp})\le q and αq(μMp)=αq(μM)\alpha_q(\mu_{Mp})=\alpha_q(\mu_M).

Proof. Lemma 1 gives κ(gC)=κ(C)\kappa(gC)=\kappa(C), and the color permutations permute the classes of ff, so Lemma 3 gives, for the classes DcD_c of the layering, ∑c∣R(Dc)∣=p∑c∣R(f−1c)∣\sum_c|R(D_c)|=p\sum_c|R(f^{-1}c)|, whence αq(μMp)≥αq(μM)\alpha_q(\mu_{Mp})\ge\alpha_q(\mu_M). The reverse inequality is the inherited nonjump recurrence (3) of the root-coverage page, αq(B⊗Sm)≤αq(B)\alpha_q(B\otimes S_m)\le\alpha_q(B), which is author-recorded there. □\square

The root-coverage page proposed amplifying τq≥1/αq\tau_q\ge1/\alpha_q by forcing αq\alpha_q to decay. Corollary 4 shows where that mechanism cannot act: αq\alpha_q cannot decrease across a prime at which some coloring attaining αq\alpha_q has a robust twisted layering, so any decay, and with it any chromatic jump forced through τq≥1/αq\tau_q\ge1/\alpha_q, happens at primes where every such coloring fails to layer robustly.

Call a twisted layering ss-robust if ⋂t∉TΣ(Ct,c)={0}\bigcap_{t\notin T}\Sigma(C_{t,c})=\{0\} for every color cc and every set TT of at most ss layers; robust means 1-robust. The layers outside such a TT are themselves a family of proper qq-colorings with trivial intersections, so an ss-robust layering with pp layers has p−s≥τq(μM)p-s\ge\tau_q(\mu_M).

Lemma 5 (localization). Let D=⋃tζptCtD=\bigcup_t\zeta_p^tC_t with dissociated layers, and let T⊊Z/pT\subsetneq\mathbb Z/p satisfy ⋂t∉TΣ(Ct)={0}\bigcap_{t\notin T}\Sigma(C_t)=\{0\}. Then for all Yt∈Z[ζM]Y_t\in\mathbb Z[\zeta_M], t∈Tt\in T,

∑t∈TζptYt∈Σ(D)  ⟺  Yt∈Σ(Ct) for every t∈T.\sum_{t\in T}\zeta_p^tY_t\in\Sigma(D) \iff Y_t\in\Sigma(C_t)\ \text{for every }t\in T.

Proof. A representation ∑tζptut\sum_t\zeta_p^tu_t with ut∈Σ(Ct)u_t\in\Sigma(C_t) differs from the given sum by a vanishing combination of the ζpt\zeta_p^t, so ut=Yt+wu_t=Y_t+w on TT and ut=wu_t=w off TT for one common ww, and w∈⋂t∉TΣ(Ct)={0}w\in\bigcap_{t\notin T}\Sigma(C_t)=\{0\}. □\square

Every value Y∈Z[ζMp]Y\in\mathbb Z[\zeta_{Mp}] has decompositions Y=∑tζptYtY=\sum_t\zeta_p^tY_t with a zero component, since subtracting one component from all of them changes nothing. Write s(Y)s(Y) for the complexity of a value, the least support of a signed representation by roots. Concatenating component representations shows s(Y)≤∑ts(Yt)s(Y)\le\sum_ts(Y_t) for every decomposition, and splitting a shortest representation by layers gives a decomposition with equality, supported on at most s(Y)s(Y) layers.

Proposition 6 (annealed transfer). Let ff be a proper qq-coloring of μM\mu_M with classes C(j)C^{(j)}, put Λ(X)=max⁡jPr⁡g[g^X∈Σ(C(j))]\Lambda(X)=\max_j\Pr_g[\hat gX\in\Sigma(C^{(j)})] for X∈Z[ζM]X\in\mathbb Z[\zeta_M] and gg uniform in GMG_M, and let the twists gtg_t of a twisted layering be independent and uniform. Let h=(h′,π)h=(h',\pi) be uniform in GMp=GM×Sym(Z/p)G_{Mp}=G_M\times\mathrm{Sym}(\mathbb Z/p) and independent of them, and let Y=∑t∈TζptYtY=\sum_{t\in T}\zeta_p^tY_t with ∣T∣≤s|T|\le s. If EE is the event that the layering is ss-robust, then for every color cc of the layering

Pr⁡[h^Y∈Σ(Dc) and E]≤∏t∈TΛ(Yt).\Pr\bigl[\hat hY\in\Sigma(D_c)\ \text{and}\ E\bigr]\le\prod_{t\in T}\Lambda(Y_t).

Proof. h^Y=∑t∈Tζpπ(t)h^′Yt\hat hY=\sum_{t\in T}\zeta_p^{\pi(t)}\hat h'Y_t. On EE, Lemma 5 reduces membership to g^π(t)h^′Yt∈Σ(C(jt))\hat g_{\pi(t)}\hat h'Y_t\in\Sigma(C^{(j_t)}) for every t∈Tt\in T, with jtj_t fixed by cc and the color permutation of layer π(t)\pi(t). Given π\pi and h′h', the elements gπ(t)h′g_{\pi(t)}h', t∈Tt\in T, are independent and uniform in GMG_M because the gπ(t)g_{\pi(t)} are. □\square

So if the twisted copies of one coloring satisfy Λ(X)≤κs(X)\Lambda(X)\le\kappa^{s(X)} for every value of complexity at most ss, the next grid inherits Pr⁡[h^Y∈Σ(Dc)]≤κs(Y)+Pr⁡[Ec]\Pr[\hat hY\in\Sigma(D_c)]\le\kappa^{s(Y)}+\Pr[E^c] for every value of complexity at most ss, on average over the twists. This is the exact form in which the race model of Section 6 transmits itself from one conductor to the next; by Lemma 7 the hypothesis can hold only for ss up to about log⁡∣GM∣/log⁡(1/κ)\log|G_M|/\log(1/\kappa). It is annealed: the first-moment count at the following prime needs the p′p'-th moment of the quenched probability, and two twisted copies of YY that use two common layers are correlated through the ratio of their twists.

5. Exact small cases

The evidence checker verifies the first three items by exact integer arithmetic.

  • μ15\mu_{15}, two colors. μ15\mu_{15} has 446 nonzero signed relations with 127 supports, of which 98 are minimal, of sizes 3, 5, 6, 7, 8 and 9; its largest dissociated sets have 8=φ(15)8=\varphi(15) elements. Its 1440 proper 2-colorings (as unordered partitions) all have classes of sizes 7 and 8, and form four orbits of 360 under G15G_{15}, of order 720. Every 8-element class spans every root, so κ=1\kappa=1. The 7-element class leaves 6 roots outside its signed span in 360 colorings and 4 roots in the other 1080.
  • Nine layers suffice. Nine labeled proper 2-colorings of μ15\mu_{15}, eight from one G15G_{15}-orbit and one from another, have trivial signed-span intersection for both colors. Hence τ2(S3⊗S5)≤9\tau_2(S_3\otimes S_5)\le9, sharpening the inherited range 8≤τ2≤108\le\tau_2\le10 of the tensor-layer test; the primes this decides are unchanged: χ(μ15p)=2\chi(\mu_{15p})=2 for every prime p≥11p\ge11.
  • Arc classes below the rank threshold span nothing outside. For M∈{105,165,195,1155,15015,255255}M\in\{105,165,195,1155,15015,255255\} and q∈{3,4}q\in\{3,4\}, an arc of ⌈M/q⌉≤φ(M)\lceil M/q\rceil\le\varphi(M) consecutive roots is part of a power basis, and no root outside it lies in its signed span, so κ=⌈M/q⌉/M\kappa=\lceil M/q\rceil/M, equal to 1/31/3 when q=3q=3. This is the smallest root-span fraction possible for an arc of that size. The largest power-basis coordinate of a root of unity grows from 2 at 105 to 545 at 15015 and 116762 at 255255.
  • Signed pairs of roots behave like independent points. For the arc class of q=3q=3 at M=105M=105 and M=1155M=1155 we computed, for each agreement pattern of a pair of distinct roots and each sign, the probability that a uniform coordinate twist sends the signed pair into the class's signed span; coordinate twists act transitively on the pairs with a given pattern. The only representations other than the obvious one are the identities z+zω=−zω2z+z\omega=-z\omega^2 on cosets of μ3\mu_3, which make such a pair a single root in disguise, surviving with probability exactly 1/31/3. Every other pattern survives with probability between 00 and 0.13330.1333, against κ2=0.1111\kappa^2=0.1111: assumption 1 of the race model holds for complexity two at these conductors, up to a factor 1.21.2.
  • Signed triples. At M=105M=105, exactly, and at M=1155M=1155, by a Monte Carlo estimate with 1500 samples per orbit, the orbits of signed triples whose values do not visibly reduce through cosets of μ3\mu_3 or μ5\mu_5 survive a random twist with probability at most 4/45≈0.0894/45\approx0.089 at 105 and about 0.0880.088 at 1155, against κ3=0.037\kappa^3=0.037. The excess sits on small orbits of triples confined to a few coordinates: at 105 every such orbit needs fewer layers than the roots, as (O) asks (log⁡∣O∣/log⁡(1/λO)\log|O|/\log(1/\lambda_O) at most 3.43.4 against 4.24.2 for the roots), and at 1155 the estimates give at most 5.65.6 against 6.46.4.
  • Two arcs fail at 165 and 195, two colors do not. Φ165\Phi_{165} and Φ195\Phi_{195} have height two while (1−x)Φ165(1-x)\Phi_{165} and (1−x)Φ195(1-x)\Phi_{195} are flat (inherited table), so D(165)=81D(165)=81 and D(195)=97D(195)=97, and L123 shows that two arcs are not proper there. The nine-layer family nevertheless gives χ(μ165)=χ(μ195)=2\chi(\mu_{165})=\chi(\mu_{195})=2. Arc colorings are therefore not optimal beyond the rank threshold.
  • Solver observations, not certificates. A direct exact-coefficient integer program found no signed relation in either class of the resulting colorings of μ165\mu_{165} and μ195\mu_{195}, while it found one in an arc of ⌈N/2⌉\lceil N/2\rceil roots and in the layering with all layers equal. In that coloring of μ165\mu_{165} the 82-element class represents at least 71 of the 83 roots outside it (each found representation was checked), and the solver found none for the other 12; the 83-element class represents at least 70 of 82, with none found for 12. Such classes are nearly maximal, and twisted layerings of this one coloring need at least ⌈165/12⌉=14\lceil165/12\rceil=14 layers if these reported representation counts hold (the counting bound of the root-coverage page), one more than the prime 13 supplies at 3⋅5⋅11⋅133\cdot5\cdot11\cdot13. The reported 12 unrepresented roots of each class lie on only 2 of the 11 values of the 11-coordinate, suggesting a further obstruction to efficient coverage by twists. A set-cover program over 20000 random candidate twists found no 17 that leave every root unspanned in some layer for both colors, and over 6000 candidates the least such family within that sample has 22 twists. These sampled searches give no global obstruction at 17 or 19 layers. The reported 22-twist family would suffice for root exclusion with 23 layers, but its solver output is not retained here as an exact certificate.

These cases fit one pattern: twisted layering struggles where the colors are tight, that is, where qq classes can cover μM\mu_M only by being nearly maximal dissociated sets, because nearly maximal classes span almost every root and slow the race below. This is the case for q=2q=2 at M=15M=15, where every 8-element class is a largest dissociated set spanning all roots and the coloring number jumps to 3 at 105, and for the coloring of μ165\mu_{165} above, whose classes leave only 12 roots unspanned.

6. The race model and its first moment

This section is a model, not an argument, except for the identity (O) and Lemma 7, which are proved.

For one color, let the layers come from a class CC of a proper qq-coloring of μM\mu_M under independent uniform twists, and write κ=κ(C)\kappa=\kappa(C). A nonzero value FF is common when g^tF∈Σ(C)\hat g_tF\in\Sigma(C) for every layer. Since g^F\hat gF is uniform on the GMG_M-orbit OO of FF, it survives one layer with probability λO=∣O∩Σ(C)∣/∣O∣\lambda_O=|O\cap\Sigma(C)|/|O|, independently, and the expected number of nonzero common values is exactly

∑O∣O∣ λO p,(O)\sum_{O}|O|\,\lambda_O^{\,p}, \tag{O}

the sum over the GMG_M-orbits of nonzero values. Orbit OO is killed in expectation once pp exceeds pO=log⁡∣O∣/log⁡(1/λO)p_O=\log|O|/\log(1/\lambda_O). The roots form an orbit of size MM with λ=κ\lambda=\kappa (Lemma 2), so they need p>log⁡M/log⁡(1/κ)p>\log M/\log(1/\kappa). Classify a value FF by its complexity s(F)s(F), the least support of a signed representation by roots of μM\mu_M. The model assumes:

  1. the roots are the binding orbits: a value of complexity ss survives one random layer with probability at most about κs\kappa^s, or more generally its orbit needs no more layers than the roots do (exact for s=1s=1; for s≥2s\ge2 it treats the points of a representation as nearly independent);
  2. at most (Ms)2s\binom Ms2^s values have complexity ss.

Under these assumptions the expected number of common nonzero values would be at most about

q∑s≥1(Ms)2sκps≤q(e2Mκp−1),q\sum_{s\ge1}\binom Ms2^s\kappa^{ps}\le q\bigl(e^{2M\kappa^p}-1\bigr),

dominated by single roots and small once

plog⁡1κ>log⁡(2qM).(R)p\log\frac1\kappa>\log(2qM). \tag{R}

The term of the single roots is exact: by Lemma 2 the roots and their negatives contribute 2Mκp2M\kappa^p per color, so (R) is exactly the condition that the roots lose the race in expectation. The rest of the bound is false at large conductors.

Lemma 7 (the first moment diverges). Let C⊆μMC\subseteq\mu_M be dissociated and let g1,…,gpg_1,\ldots,g_p, with p≥2p\ge2, be independent and uniform in GMG_M. Then

E #{F≠0:g^tF∈Σ(C) for every t} ≥ 2∣C∣−1∣GM∣ p−1.\mathbb E\,\#\{F\ne0:\hat g_tF\in\Sigma(C)\ \text{for every}\ t\} \ \ge\ \frac{2^{|C|}-1}{|G_M|^{\,p-1}}.

Proof. By (O) in the form of Section 8, the expectation is ∑0≠F∈Σ(C)λ(F)p−1\sum_{0\ne F\in\Sigma(C)}\lambda(F)^{p-1}. For F∈Σ(C)F\in\Sigma(C) the orbit OO of FF meets Σ(C)\Sigma(C) at least in FF, so λ(F)≥1/∣O∣≥1/∣GM∣\lambda(F)\ge1/|O|\ge1/|G_M|; and ∣Σ(C)∣≥2∣C∣|\Sigma(C)|\ge2^{|C|}, because the subset sums of a dissociated set are distinct. □\square

One event carries the bound: with probability ∣GM∣1−p|G_M|^{1-p} all twists are equal, and then every element of Σ(C)\Sigma(C) is common. For the odd-prime grids ∣GNk∣=∏i≤kpi!|G_{N_k}|=\prod_{i\le k}p_i!, so log⁡∣GNk∣\log|G_{N_k}| grows like pk2/2p_k^2/2, while the largest class of a proper qq-coloring has at least Nk/q=e(1+o(1))pk/qN_k/q=e^{(1+o(1))p_k}/q elements. Hence for every fixed qq the right side of Lemma 7 tends to infinity along the grids. Exactly, with p=pk+1p=p_{k+1}: a class of ⌈M/2⌉\lceil M/2\rceil elements gives an expectation above 2122^{12} at M=1155M=1155, and classes of ⌈M/q⌉\lceil M/q\rceil elements give expectations above 224792^{2479} at M=15015M=15015 for q=2,3,4q=2,3,4; at M=1155M=1155 the bound says nothing for q=3q=3. Three consequences:

  • Assumption 1 fails for every F∈Σ(C)F\in\Sigma(C) whose complexity exceeds log⁡∣GM∣/log⁡(1/κ)\log|G_M|/\log(1/\kappa), since such FF have λ(F)≥1/∣GM∣>κs(F)\lambda(F)\ge1/|G_M|>\kappa^{s(F)}. At most ∑j≤s(Mj)2j\sum_{j\le s}\binom Mj2^j values have complexity at most ss, so most of Σ(C)\Sigma(C) is of this kind once ∣C∣|C| is large.
  • For any fixed palette, the unconditioned union bound over individual common values cannot certify properness at all sufficiently large odd-prime orders. The exact bound already exceeds one at M=15015M=15015 for the tested palettes q=2,3,4q=2,3,4.
  • Lemma 7 does not show that twisted layerings fail. The expectation is carried by twist families of tiny probability, such as families of equal twists; it shows only that the first moment cannot certify properness.

What survives. The race of the roots is exact, and so is any first-moment count restricted to values of complexity at most s0s_0, where the degenerate events of Lemma 7 contribute at most ∑j≤s0(Mj)2j ∣GM∣1−p\sum_{j\le s_0}\binom Mj2^j\,|G_M|^{1-p}, negligible while s0log⁡(2eM)s_0\log(2eM) stays well below (p−1)log⁡∣GM∣(p-1)\log|G_M|, an allowance of order (log⁡M)2(\log M)^2 for the odd-prime grids. A proof of properness along this route therefore splits in two: the first moment over values of complexity at most s0s_0, which the model's assumptions address, and a rigidity statement, that outside an event of small probability the twists have no common value of complexity above s0s_0. The second part cannot come from a union bound over values; Section 7 states it.

Primes. For the odd-prime grids take M=Nk=3⋅5⋯pkM=N_k=3\cdot5\cdots p_k and p=pk+1p=p_{k+1}, so log⁡Nk=θ(pk)−log⁡2\log N_k=\theta(p_k)-\log2 with Chebyshev's function θ\theta. Since θ(x)∼x\theta(x)\sim x and pk+1>pkp_{k+1}>p_k, (R) holds for every large kk when κ<e−1\kappa<e^{-1}, up to a factor 1+o(1)1+o(1) in the exponent. With κ=1/3\kappa=1/3 the margin is

pk+1log⁡3−log⁡(6Nk)≥(log⁡3−1.01624) pk−log⁡3,p_{k+1}\log3-\log(6N_k)\ge(\log3-1.01624)\,p_k-\log3,

by the explicit bound θ(x)<1.01624 x\theta(x)<1.01624\,x for x>0x>0 of Rosser and Schoenfeld (1962). The right side grows linearly and is positive for pk≥17p_k\ge17; direct computation shows that the margin itself is positive for every pk≥3p_k\ge3. So the expected numbers of surviving roots are summable over kk; by Lemma 7 the full first moment is not. Three arcs are proper by the rank bound through the prime 19, with κ=1/3\kappa=1/3 exactly (Section 5, computed through 255255255255), and their roots lose the race at 23 and at every later prime; whether twisted layerings of them stay proper depends on the rigidity statement. Two colors lose even the root race for every large kk, since log⁡2<1\log2<1, consistent with χ(μ105)=3\chi(\mu_{105})=3.

Other side schedules. For simplex tensors with sides qj=Ajlog⁡jq_j=Aj\log j the same computation gives log⁡Mj∼jlog⁡j\log M_j\sim j\log j and qj∼Alog⁡Mjq_j\sim A\log M_j, so (R) holds eventually when κ<e−1/A\kappa<e^{-1/A}. The inherited extraction loss Q/(2qj2)Q/(2q_j^2) of the tensor extraction theorem has log⁡Q∼∑i<j(log⁡qi)/qi∼(log⁡j)/A\log Q\sim\sum_{i<j}(\log q_i)/q_i\sim(\log j)/A, so it is summable only for A≥1A\ge1. For every schedule that the inherited extraction method covers, roughly e1/A+1e^{1/A}+1 colors win the root race; the primes sit at A=1A=1. The root race therefore does not distinguish the side schedules, and Lemma 7 applies to all of them.

Where the model can fail.

  • Tightness. If every proper qq-coloring of some μNk\mu_{N_k} has nearly maximal classes, κ\kappa is close to 1 and (R) fails; this is how the small jumps happen. The model needs qq to exceed the fractional coloring number Nk/Ψ(Nk)N_k/\Psi(N_k) with room to spare. L21 bounds that fractional number uniformly, but its constant is not explicit.
  • Values with many short representations. Inflations of short relations of subconductors, and other structured values, can have survival probabilities far above κs\kappa^s. For arc classes, the fiber geometry removes the most obvious ones: every coset of μ3\mu_3 meets an arc of length N/3N/3 exactly once, and coordinate twists map such cosets to such cosets.
  • Correlations between the classes of the base coloring.

7. Consequences for the attack

  • The open claim. χ(μN)≤3\chi(\mu_N)\le3 for every odd squarefree NN, hence χ(μ∞)≤6\chi(\mu_\infty)\le6 by the inherited reduction, a positive answer to Déchamps's Question 38, and (4) false. It is recorded as the open claim L210, which states exactly this bound. Three colors win the root race at every prime, but by Lemma 7 that is the only part of the first-moment count that holds, so the claim is a conjecture supported by the root race, the rank bound through seven primes and small-order data. It is independent of L124: two arcs already fail at 165 while two colors succeed.
  • What a proof of (4) must do. For every palette qq it must find a prime at which no family of proper qq-colorings of the previous grid, twisted or not, has trivial signed-span intersections; by Corollary 4, if the jump is to come from decay of the root coverage, that prime must defeat robust twisted layerings of the colorings attaining αq\alpha_q. Since the roots lose their race, it needs tightness at infinitely many conductors for every fixed palette, or common values of complexity at least two that survive typical twist families. Lemma 7 does not supply the latter: it exhibits common values only on twist families of tiny probability.
  • What a proof of the open claim needs. Two parts, with a threshold s0s_0 inside the allowance of Section 6. First, for values of complexity at most s0s_0, a bound of the form Pr⁡g[g^F∈Σ(C)]≤κc s(F)\Pr_g[\hat gF\in\Sigma(C)]\le\kappa^{c\,s(F)}, uniform in the conductor, for the classes CC produced by robust twisted layerings, together with a count of the relevant orbits. With the crude count in assumption 2 and p∼log⁡Mp\sim\log M, the exponent must satisfy clog⁡(1/κ)>1c\log(1/\kappa)>1; an unspecified c>0c>0 is insufficient. The error probabilities from this estimate and the rigidity estimate must sum to less than one over all colors and all required robustness tests. Lemma 3 already transfers κ\kappa itself exactly, and Section 5 supports the bound for complexity two and three at small conductors. By Lemma 7 no such bound can hold for every FF: it fails for each F∈Σ(C)F\in\Sigma(C) of complexity above log⁡∣GM∣/(clog⁡(1/κ))\log|G_M|/(c\log(1/\kappa)). Second, rigidity: outside an event of small probability, a family of pp independent uniform twists has no common value of complexity above s0s_0. The exceptional event must contain the near-coincident families behind Lemma 7, and the statement has to explain how a value can have signed representations inside many twisted copies of one class, which no count over values does. Lemma 9 of Section 10 reduces it to a property of a single class: the survival sets of its values of large complexity, apart from few orbits, must be covered by fewer than pp translates of a small set of twists (fewer than p/qp/q if the color permutations distribute the classes over the layers).
  • Tests that can falsify the model. τ2(μ165)\tau_2(\mu_{165}), which decides χ(μ3⋅5⋅11⋅13)\chi(\mu_{3\cdot5\cdot11\cdot13}); the root-span fraction of other proper 2-colorings of μ165\mu_{165}; survival of values of complexity three and more for arc classes; and κ\kappa of arc classes at 4849845=3⋅5⋯194849845=3\cdot5\cdots19, the last conductor where three arcs are below the rank threshold.

8. Shape of the missing estimate

Write λ(F)=λO\lambda(F)=\lambda_O for the orbit OO of FF. Since ∣O∣λO=∣O∩Σ(C)∣|O|\lambda_O=|O\cap\Sigma(C)|, the identity (O) can be rewritten as a sum over the class's own signed sums,

E #{nonzero common values}=∑0≠F∈Σ(C)λ(F)p−1,\mathbb E\,\#\{\text{nonzero common values}\} =\sum_{0\ne F\in\Sigma(C)}\lambda(F)^{p-1},

and since λ(F)≥1/∣GM∣\lambda(F)\ge1/|G_M| on Σ(C)\Sigma(C) the right side is at least (∣Σ(C)∣−1)/∣GM∣p−1(|\Sigma(C)|-1)/|G_M|^{p-1}, which is Lemma 7. No signed sum of CC has an orbit of which Σ(C)\Sigma(C) occupies a fraction below 1/∣GM∣1/|G_M|, so the estimate can only concern values of small complexity, as Section 7 states. For those, since g^F∈Σ(C)\hat gF\in\Sigma(C) exactly when some signed representation RR of FF has g(supp⁡R)⊆Cg(\operatorname{supp}R)\subseteq C,

λ(F)≤∑Rπ(supp⁡R),π(S)=Pr⁡g[gS⊆C],\lambda(F)\le\sum_{R}\pi(\operatorname{supp}R),\qquad \pi(S)=\Pr_g[gS\subseteq C],

the sum running over all signed representations of FF. For an arc class the natural survival π(S)\pi(S) trades off against the orbit size of SS: a support confined to few coordinate values has a small orbit, and each new coordinate value placed last in a coordinate of a prime rr must land in a set of about r/3r/3 of the rr residues. For large complexity the count of representations is not the obstacle. The far-regime model of the angular-coloring page gives a typical value about A(α)tA(\alpha)^t representations of support t=αMt=\alpha M, with A(α)=2exp⁡((H(α)−e−γ)/α)≤2.66A(\alpha)=2\exp\bigl((H(\alpha)-e^{-\gamma})/\alpha\bigr)\le2.66 for the binary entropy HH in nats, below the factor 3t3^t; but natural survival does not pay 3−t3^{-t} once 3t3^t exceeds ∣GM∣|G_M|. The coordinate-permutation group has only ∏ipi!=eO((log⁡M)2)\prod_ip_i!=e^{O((\log M)^2)} elements while ∣Σ(C)∣|\Sigma(C)| is exponential in MM, so a single representation inside CC already gives λ(F)≥1/∣GM∣\lambda(F)\ge1/|G_M|, and the large-complexity part must come from the rigidity statement of Section 7.

9. Certificates by pairs of layers stay below the rank

The layer criterion certifies dissociation recursively. For odd squarefree NN and a prime p∣Np\mid N, write each S⊆μNS\subseteq\mu_N as S=⋃t∈Z/pζptStS=\bigcup_{t\in\mathbb Z/p}\zeta_p^tS_t with St⊆μN/pS_t\subseteq\mu_{N/p}. Call SS pair-certified if either NN is prime and S≠μNS\ne\mu_N, or for some prime p∣Np\mid N every layer StS_t is pair-certified and either some layer is empty or some two layers Sa,SbS_a,S_b with a≠ba\ne b are disjoint and Sa∪SbS_a\cup S_b is pair-certified. The prime may change from step to step.

Lemma 8. Every pair-certified S⊆μNS\subseteq\mu_N is dissociated and has at most φ(N)\varphi(N) elements.

Proof. Induction on the number of prime factors of NN. For NN prime the only nonzero signed relations of μN\mu_N are the sum of all its elements and its negative, so S≠μNS\ne\mu_N is dissociated and ∣S∣≤N−1=φ(N)|S|\le N-1=\varphi(N). Otherwise the layers are dissociated by induction. If SaS_a and SbS_b are disjoint with dissociated union, a common value w=ua=ubw=u_a=u_b with ua∈Σ(Sa)u_a\in\Sigma(S_a) and ub∈Σ(Sb)u_b\in\Sigma(S_b) gives the signed relation ua−ub=0u_a-u_b=0 of Sa∪SbS_a\cup S_b, so w=0w=0; an empty layer has Σ(St)={0}\Sigma(S_t)=\{0\}. Either way ⋂tΣ(St)={0}\bigcap_t\Sigma(S_t)=\{0\}, and SS is dissociated by the layer criterion. For the size, ∣S∣≤(p−2)φ(N/p)+∣Sa∪Sb∣≤(p−1)φ(N/p)=φ(N)|S|\le(p-2)\varphi(N/p)+|S_a\cup S_b|\le(p-1)\varphi(N/p)=\varphi(N), and an empty layer gives the same bound. □\square

The two simplest ways of making the common-value intersection trivial, an empty layer or two layers with dissociated union, never certify a set beyond the rank, whichever primes are used. A proper qq-coloring with q<N/φ(N)q<N/\varphi(N) has a class larger than φ(N)\varphi(N). Since two dissociated sets have trivially intersecting signed spans exactly when they are disjoint with dissociated union, any recursive certification of such a class must, at some step, show that three or more signed spans intersect trivially although no two of them do. Coloring beyond the rank is in this sense a higher-order phenomenon: the nine-layer family of Section 5 shrinks the intersection only gradually (447 values remain after two layers), and twisted layerings rely on intersections over many layers. This is also why the rigidity statement of Section 7 concerns many twisted copies at once.

10. Clustered survival sets

Lemma 7 says that a union bound over values fails; the following lemma shows how values can be excluded together instead. For a class CC and a nonzero value FF write

T(F)={g∈GM:g^F∈Σ(C)},T(F)=\{g\in G_M:\hat gF\in\Sigma(C)\},

the survival set of FF, so that λ(F)=∣T(F)∣/∣GM∣\lambda(F)=|T(F)|/|G_M| and FF is common to the layers of a twisted layering of CC exactly when every twist lies in T(F)T(F). Fix a set N⊆GM\mathcal N\subseteq G_M containing the identity and call FF mm-clustered if T(F)T(F) is covered by at most mm left translates hNh\mathcal N.

Lemma 9. Let g1,…,gpg_1,\ldots,g_p be independent and uniform in GMG_M and m<pm<p. The probability that some mm-clustered value is common to all pp layers is at most (p2)∣N−1N∣/∣GM∣\binom p2|\mathcal N^{-1}\mathcal N|/|G_M|.

Proof. If an mm-clustered FF is common, the pp twists lie in T(F)T(F), which is covered by m<pm<p translates of N\mathcal N, so two of them, gsg_s and gtg_t with s≠ts\ne t, lie in one translate and gs−1gt∈N−1Ng_s^{-1}g_t\in\mathcal N^{-1}\mathcal N. For s≠ts\ne t the element gs−1gtg_s^{-1}g_t is uniform on GMG_M; take the union over the (p2)\binom p2 pairs. □\square

The bound does not sum over values, and it absorbs the degenerate events of Lemma 7, in which twists coincide. A random twisted layering is therefore proper with probability at least 1−ε1-\varepsilon as soon as, for some N\mathcal N with $\binom p2|\mathcal N^{-1}\mathcal N|\le \varepsilon|G_M|/2$ and some m<pm<p, the first moment of the common values that are not mm-clustered, summed over the classes, is at most ε/2\varepsilon/2. This is the case where every color permutation σt\sigma_t of Section 3 is the identity, so that each color uses twisted copies of one class; if the color permutations distribute the qq classes evenly over the layers, the same argument applies with m<p/qm<p/q clusters per class. This replaces the rigidity statement of Section 7 by a property of a single class: its unclustered values must be few enough for a first moment.

Which values are unclustered depends on their representations, since T(F)T(F) is the union, over the signed representations RR of FF, of the sets of twists carrying supp⁡R\operatorname{supp}R into CC with matching signs. In the following list the descriptions of T(F)T(F) are exact and the counts are heuristic.

  • Roots and short values. A root yy has ∣T(y)∣=κ∣GM∣|T(y)|=\kappa|G_M|, spread over the whole group, and values of small complexity are similar; they are the first-moment part, exact for the roots by Lemma 2.
  • Thin supports. If a representation of FF lies in a box ∏iAi\prod_iA_i with small sides, T(F)T(F) is a union of left cosets of the large group ∏iSym(Z/pi∖Ai)\prod_i\mathrm{Sym}(\mathbb Z/p_i\setminus A_i), which fixes the box pointwise, so FF is not clustered for any small N\mathcal N; such values fall into comparatively few orbits, and the first moment is the tool for them.
  • A unique representation. If FF has a single signed representation, with support SS, then T(F)={g:gS⊆C}T(F)=\{g:gS\subseteq C\} up to sign compatibility. A maximal family of elements of T(F)T(F) with pairwise ha−1hb∉N−1Nh_a^{-1}h_b\notin\mathcal N^{-1}\mathcal N covers T(F)T(F) by its translates of N−1N\mathcal N^{-1}\mathcal N, so FF fails to be mm-clustered for N−1N\mathcal N^{-1}\mathcal N only if SS lies in m+1m+1 twisted copies h0−1C,…,hm−1Ch_0^{-1}C,\ldots,h_m^{-1}C of the class with such pairwise far twists. For twisted copies that intersect like independent sets of density 1/q1/q, m+1m+1 copies share about Mq−m−1Mq^{-m-1} points, fewer than the complexity threshold once m+1m+1 exceeds about log⁡qM\log_q M; that is below pp exactly in the regime (R) where the roots lose their race.
  • Many representations. The open case is a value of large complexity whose representations land in many pairwise far copies of CC. Their differences are integer relations with coefficients in {−2,−1,0,1,2}\{-2,-1,0,1,2\}, and need not be ternary relations. Suppose that CC meets every line of direction pp in at most ⌈p/q⌉\lceil p/q\rceil points, as twisted arc classes do, and that FF has a representation inside CC. A twist maps lines onto lines, so the twisted representation also meets every line in at most ⌈p/q⌉\lceil p/q\rceil points, and the only relations supported on one line are the multiples of its indicator: changing the representation along a single line leaves at least p−⌈p/q⌉>⌈p/q⌉p-\lceil p/q\rceil>\lceil p/q\rceil points of that line in the new support when q≥3q\ge3, too many for CC. So the relations that carry a twisted representation back into CC involve at least two lines; longer relations are not controlled. At the conductor 105 the relations that carry a twisted image back into the arc class lie on two or three grid lines: crosses and stars built from the identities ∑x∈ℓ∖Px=−∑x∈Px\sum_{x\in\ell\setminus P}x=-\sum_{x\in P}x for a line ℓ\ell and a set PP of its points.

The single-class property to prove is therefore: for the classes of the colorings being layered, a set N\mathcal N of twists with ∣N−1N∣≤∣GM∣/p3|\mathcal N^{-1}\mathcal N|\le|G_M|/p^3, such that every value of complexity above s0s_0 that is not in a few orbits of thin or short values has its survival set covered by fewer than pp translates of N\mathcal N. That threshold is for layerings that keep each color on twisted copies of one class, with every color permutation σt\sigma_t the identity; if the color permutations distribute the classes evenly over the layers, it is p/qp/q.

The set N\mathcal N cannot consist only of twists that move few points. For the arc class C={ζe:0≤e<M/3}C=\{\zeta^e:0\le e<M/3\}, every value supported on the initial arc {ζe:0≤e<M/(3m)}\{\zeta^e:0\le e<M/(3m)\} survives each Galois automorphism ζ↦ζu\zeta\mapsto\zeta^u with u≤mu\le m a unit modulo MM, because ue<M/3ue<M/3 there; these automorphisms move almost every point, and the values have complexity up to about M/(3m)M/(3m), far above s0s_0 when m≈pm\approx p. The cyclotomic symmetries ζe↦ζue+d\zeta^e\mapsto\zeta^{ue+d} are the coordinatewise affine maps, a subgroup of GMG_M of order Mφ(M)M\varphi(M), so the natural candidate is that subgroup combined with twists that move few points: a permutation of Z/r\mathbb Z/r fixing all but ηr\eta r points is one of at most (rηr)(ηr)!≤rηr\binom r{\eta r}(\eta r)!\le r^{\eta r} such permutations, against r!r! in all, so both parts are vanishing fractions of GMG_M. Families of twists whose effects on the arc parameter form an arithmetic progression keep large common parts of the arc class, and the Galois automorphisms are the basic example; whether the twists of each coordinate in such a family must be affine is part of the open question. This intersection property is open; nothing on this page proves it for any class beyond the rank.

The arc colorings sit at the clustered extreme. Write ζMp=ζMαζpβ\zeta_{Mp}=\zeta_M^{\alpha}\zeta_p^{\beta} with αp+βM=1\alpha p+\beta M=1, so that ζMpe=ζMαeζpβe\zeta_{Mp}^e=\zeta_M^{\alpha e}\zeta_p^{\beta e}. The exponents e<Mp/qe<Mp/q with βe≡t(modp)\beta e\equiv t\pmod p form a progression of difference pp, and αp≡1(modM)\alpha p\equiv1\pmod M, so layer tt of the arc coloring of μMp\mu_{Mp} is an arc of consecutive roots of μM\mu_M, of length about M/qM/q. The arc coloring is therefore the layering of the arc coloring of μM\mu_M whose twists are rotations, a subgroup of order MM, and Lemma 9 says nothing about it; its properness is decided by the cyclotomic criterion of L123 instead. That two arcs fail at 165 while twisted layerings with spread-out twists succeed is consistent with this.

At the other extreme, the support of a value is the whole arc class, and there the clustering holds exactly.

Lemma 10 (the arc has two coordinate symmetries). Let MM be odd and squarefree and A={ζMe:0≤e<L}A=\{\zeta_M^e:0\le e<L\} with 2≤L≤M−22\le L\le M-2. For a prime p∣Mp\mid M put K=M/pK=M/p and write L=aK+bL=aK+b with 0≤b<K0\le b<K. Suppose that for every prime p≥5p\ge5 dividing MM either b≥pb\ge p and 2≤a+1≤p−22\le a+1\le p-2, or K−b≥pK-b\ge p and 2≤a≤p−22\le a\le p-2. Then the coordinate permutations gg with gA=AgA=A are exactly the identity and the reflection ζe↦ζL−1−e\zeta^e\mapsto\zeta^{L-1-e}. For L=⌈M/3⌉L=\lceil M/3\rceil the hypothesis holds when M/5≥7M/5\ge7 if 5∣M5\mid M and M/p≥2pM/p\ge2p for every prime p≥7p\ge7 dividing MM, in particular for M=3⋅5⋯pkM=3\cdot5\cdots p_k with k≥3k\ge3.

Proof. Identify μM\mu_M with Z/M\mathbb Z/M by exponents. Fix a prime p∣Mp\mid M and let ww be the inverse of KK modulo pp. A line of direction pp is a coset c+KZ/Mc+K\mathbb Z/M with 0≤c<K0\le c<K; its point c+tKc+tK has pp-coordinate v≡c+tKv\equiv c+tK, so t≡w(v−c)(modp)t\equiv w(v-c)\pmod p. In the rescaled coordinate v′=wvv'=wv the points of the line inside AA, those with c+tK<Lc+tK<L, therefore form the arc [wc,wc+nc)[wc,wc+n_c) of Z/p\mathbb Z/p, with nc=a+1n_c=a+1 for c<bc<b and nc=an_c=a for b≤c<Kb\le c<K. Since pp consecutive values of cc give every rotation wcwc, the hypothesis supplies a length λ\lambda with 2≤λ≤p−22\le\lambda\le p-2 such that every arc of length λ\lambda is the trace of AA on some line. A coordinate permutation gg maps lines of direction pp onto lines of direction pp, acting on their pp-coordinates by one permutation, which in rescaled coordinates is a permutation GG of Z/p\mathbb Z/p. If gA=AgA=A, then GG maps every arc of length λ\lambda onto an arc of length λ\lambda. Passing to complements if λ>p/2\lambda>p/2, two arcs of length λ≤p/2\lambda\le p/2 share λ−1≥1\lambda-1\ge1 points exactly when their starting points differ by ±1\pm1, so the starting points transform by an automorphism r↦±r+cr\mapsto\pm r+c of the pp-cycle, and the point rr, the difference of the arcs starting at rr and r+1r+1, goes to ±r+c′\pm r+c'. Hence gg acts on the pp-coordinate by v↦±v+dpv\mapsto\pm v+d_p; for p=3p=3 every permutation has this form. So gg is e↦ue+de\mapsto ue+d on Z/M\mathbb Z/M with u2≡1u^2\equiv1, and uA+d=AuA+d=A. If L<M/2L<M/2, this map sends A∩(A+1)A\cap(A+1), of size L−1L-1, onto A∩(A+u)A\cap(A+u), of size max⁡(0,L−min⁡(u,M−u))\max(0,L-\min(u,M-u)) for the representative 0≤u<M0\le u<M, so u≡±1u\equiv\pm1; if L>M/2L>M/2 the same argument applies to the complement of AA, an interval of length M−L≥2M-L\ge2. Finally d=0d=0 when u=1u=1 and d=L−1d=L-1 when u=−1u=-1. For L=⌈M/3⌉L=\lceil M/3\rceil: at p=5p=5, a=1a=1 and b=⌈2K/3⌉≥5b=\lceil2K/3\rceil\ge5 once K≥7K\ge7; at p≥7p\ge7, both aa and a+1a+1 lie in [2,p−2][2,p-2] and max⁡(b,K−b)≥K/2≥p\max(b,K-b)\ge K/2\ge p. □\square

So a signed sum over the whole class survives, with its own support, exactly two twists, both affine. Lemma 10 concerns this natural survival only; a value can also survive a twist that carries its support off the class, through another signed representation.

The evidence checker computes survival sets at M=105M=105 for the arc class of 35 roots exhaustively over all 36288003628800 twists. The sums of the whole class, with all signs +1+1 and with alternating signs, survive exactly the identity and the reflection, with no other survivor. Twelve seeded signed sums on 20, 22 and 24 points of the class have survival sets meeting at most eight of the 720 left cosets of the affine group, fewer than 11, the next prime, which is what Lemma 9 needs for the step to 1155. Four seeded sums on 10 points meet 29 to 415 cosets, and among ten seeded sums on 17 points one meets 15 cosets and one survives two twists that move its support off the class, each through a relation on two grid lines. In these samples a survival set meeting 11 or more cosets occurs only for sums on at most 17 points, inside the first-moment allowance of Section 6 for p=11p=11, about 23 points at this conductor.

The classes that a twisted layering produces are more rigid than arcs. The checker layers the three arcs of μ15\mu_{15} by seven seeded twists into a proper and robust 3-coloring of μ105\mu_{105}, whose classes are linearly independent sets of 35 roots. The sum of each whole class survives only the identity, with neither the reflection nor any other twist; six seeded signed sums on 20 class points survive at most two twists each, and six on 10 points survive 52 to 165 each. Thus the sampled large-support values cluster with N={1}\mathcal N=\{1\} for classes of the kind the induction feeds to the next step. This finite sample gives no clustering theorem for every value in those classes. Whether that pattern persists, with spread survival only below an allowance of order (log⁡M)2(\log M)^2, is the clustering question at larger conductors.

The whole-class part of this rigidity propagates through the induction. Write Stab(C)={g∈GM:gC=C}\mathrm{Stab}(C)=\{g\in G_M:gC=C\}.

Lemma 11 (layered classes are rigid). Let C⊆μMC\subseteq\mu_M, let pp be a prime not dividing MM, and let D=⋃t∈Z/pζpt gt−1CD=\bigcup_{t\in\mathbb Z/p}\zeta_p^t\,g_t^{-1}C with twists gt∈GMg_t\in G_M. A twist h=(h′,π)h=(h',\pi) of GMp=GM×Sym(Z/p)G_{Mp}=G_M\times\mathrm{Sym}(\mathbb Z/p) satisfies hD=DhD=D exactly when h′∈gπ(t)−1Stab(C) gth'\in g_{\pi(t)}^{-1}\mathrm{Stab}(C)\,g_t for every tt. Hence Stab(D)={1}\mathrm{Stab}(D)=\{1\} when the conjugates gt−1Stab(C) gtg_t^{-1}\mathrm{Stab}(C)\,g_t have trivial common intersection and, for every permutation π≠1\pi\ne1 of Z/p\mathbb Z/p, the sets gπ(t)−1Stab(C) gtg_{\pi(t)}^{-1}\mathrm{Stab}(C)\,g_t, t∈Z/pt\in\mathbb Z/p, have no common element.

Proof. The twist hh sends the layer ζpt gt−1C\zeta_p^t\,g_t^{-1}C to ζpπ(t)h′gt−1C\zeta_p^{\pi(t)}h'g_t^{-1}C, so hD=DhD=D exactly when h′gt−1C=gπ(t)−1Ch'g_t^{-1}C=g_{\pi(t)}^{-1}C for every tt, that is, gπ(t)h′gt−1∈Stab(C)g_{\pi(t)}h'g_t^{-1}\in\mathrm{Stab}(C). For π=1\pi=1 the conditions put h′h' in every conjugate, so h′=1h'=1; for π≠1\pi\ne1 they have no common solution. □\square

Both hypotheses ask the twists to avoid coincidences: for π≠1\pi\ne1, that no single h′h' satisfies pp coset conditions at once, and for π=1\pi=1, that the conjugates of the small group Stab(C)\mathrm{Stab}(C) by different twists share no nontrivial element. Starting from an arc class, whose stabilizer has two elements by Lemma 10, and twists that avoid these coincidences at every step, every layered class has trivial stabilizer, so the sum of a whole layered class survives, with its own support, only the identity; the checker confirms this for the seeded layering at 105, whose base arcs of μ15\mu_{15} lie outside the range of Lemma 10. A quantitative bound for random twists involves the centralizers of the elements of Stab(C)\mathrm{Stab}(C) and is not written here. Large proper subsets and other representations are not covered by this argument.