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Polynomial flat representations and their extraction cost


Standing

The identity below is genuinely coefficient-safe and can preserve an actual color after profile focusing. It is not an extraction-preserving color amplifier. The focused progression already has a ternary relation inside one fiber, independently of any seed, and the full fibers have vanishing extraction in the required parameter regimes.

The critical moment palette-height theorem therefore remains unflattened within a uniformly extracting family.

1. Exact common-moment representations

Fix t≥1t\geq1, and write

wt(j)=(1,j,…,jt),b=2t+1.w_t(j)=(1,j,\ldots,j^t),\qquad b=2^{t+1}.

For s≥0s\geq0 and h≥1h\geq1, define

Ps(z)=∏i=0t(1−z2ibs),Rh(z)=∑s=0h−1(1−Ps(z)),R0=0.(1)P_s(z)=\prod_{i=0}^t(1-z^{2^i b^s}),\qquad R_h(z)=\sum_{s=0}^{h-1}(1-P_s(z)),\qquad R_0=0. \tag{1}

Binary subset sums are distinct, so PsP_s has coefficients ±1\pm1 at precisely the exponents mbsmb^s, 0≤m<b0\leq m<b. Its constant coefficient is one. The nonconstant supports of 1−Ps1-P_s lie in

[bs,(b−1)bs],[b^s,(b-1)b^s],

which are disjoint for different ss. Thus RhR_h is flat, has constant coefficient zero, and degree (b−1)bh−1(b-1)b^{h-1}.

Each PsP_s has a zero of order t+1t+1 at z=1z=1. If Rh(z)=∑mrh(m)zmR_h(z)=\sum_m r_h(m)z^m, evaluation of Euler derivatives gives

∑mrh(m)=h,∑mrh(m)mj=0(1≤j≤t).\sum_m r_h(m)=h,\qquad \sum_m r_h(m)m^j=0\quad(1\leq j\leq t).

By the binomial theorem, for all integers a,da,d,

∑mrh(m)wt(a+dm)=h wt(a).(2)\boxed{\sum_m r_h(m)w_t(a+dm)=h\,w_t(a).} \tag{2}

2. What complete-profile focusing does and does not prove

Let A=(av)v∈VA=(a_v)_{v\in V} be a finite family of nonzero integer vectors, n=∣V∣n=|V|, and suppose every qq-coloring of AA has a monochromatic nonzero relation of height at most HH. Set

T=1+(b−1)bH−1,Bt,L(A)={av⊗wt(j):v∈V,0≤j<L}.T=1+(b-1)b^{H-1},\quad B_{t,L}(A)=\{a_v\otimes w_t(j):v\in V, 0\leq j<L\}.

Take LL at least a van der Waerden threshold for qnq^n colors and progression length TT. In an arbitrary qq-coloring of these indexed columns, color jj by its complete vector of type colors. A progression a,a+d,…,a+(T−1)da,a+d,\ldots,a+(T-1)d, d>0d>0, has a constant profile. Its type colors give a monochromatic seed relation uu. Formula (2) makes

f(v,a+dm)=sgn⁡(uv)r∣uv∣(m)f(v,a+dm)=\operatorname{sgn}(u_v)r_{|u_v|}(m)

a nonzero ternary relation in one actual color. The tensor sum is (∑vuvav)⊗wt(a)=0(\sum_vu_va_v)\otimes w_t(a)=0. Distinct nonzero seed vectors give distinct lifted vectors: the first moment coordinate determines ava_v, and the degree-one coordinate then determines jj.

However, T≥bT\geq b. The coefficients of P0P_0, on the first bb nodes of that progression, already annihilate every degree-at-most-tt moment. They give a monochromatic ternary relation in any one type's fiber. The seed's relation and height hypothesis are unnecessary for color forcing in this construction. This correction was identified by a separate reviewer and is part of the current standing.

The finite progression statement was checked, after the supplied digest, in Graham--Rothschild, Corollary 8. No other Ramsey theorem is being substituted for its exact conclusion.

3. Full fibers destroy uniform extraction

For any nonzero ava_v, its fiber is linearly isomorphic to

Wt(L)={wt(j):0≤j<L}.W_t(L)=\{w_t(j):0\leq j<L\}.

If D⊆Wt(L)D\subseteq W_t(L) is dissociated, all 2∣D∣2^{|D|} subset sums are distinct. Coordinate ℓ\ell, 0≤ℓ≤t0\leq\ell\leq t, has integer values between zero and Lℓ+1L^{\ell+1}. Therefore

2∣D∣≤∏ℓ=0t(Lℓ+1+1)≤(L+1)(t+22),2^{|D|}\leq\prod_{\ell=0}^t(L^{\ell+1}+1) \leq(L+1)^{\binom{t+2}2},

and consequently

η(Bt,L(A))≤(t+22)log⁡2(L+1)L.(3)\boxed{\eta(B_{t,L}(A))\leq \binom{t+2}2\frac{\log_2(L+1)}L.} \tag{3}

This upper bound uses one genuine subset of the lift, so an arbitrarily good seed cannot remove the obstruction.

For the displayed representations, L≥T≥2(t+1)(H−1)L\geq T\geq2^{(t+1)(H-1)}. Writing u=t+1≥2u=t+1\geq2, monotonicity of log⁡2(x+1)/x\log_2(x+1)/x bounds (3) by

u2[u(H−1)+1]2−u(H−1).u^2[u(H-1)+1]2^{-u(H-1)}.

For H≥4H\geq4 this is decreasing in u≥2u\geq2: its logarithmic derivative is at most 3/u−(H−1)log⁡2<03/u-(H-1)\log2<0. Thus

η(Bt,L(A))≤4(2H−1)4−(H−1)⟶0,(4)\eta(B_{t,L}(A))\leq4(2H-1)4^{-(H-1)}\longrightarrow0, \tag{4}

uniformly in the chosen degree t≥1t\geq1.

A loss for any complete-profile progression implementation

A uniformly random QQ-coloring of [0,L−1][0,L-1] has expected number of monochromatic length-TT progressions at most L2Q1−TL^2Q^{1-T}. If this is less than one, some coloring avoids them all. Universal progression focusing therefore requires

L≥Q(T−1)/2.(5)L\geq Q^{(T-1)/2}. \tag{5}

For a flat representation of h wt(0)h\,w_t(0), h≥2h\geq2, using the nodes 0,…,T−10,\ldots,T-1, one must have T≥t+2T\geq t+2. Otherwise their Vandermonde columns are independent, whereas subtracting the target gives a nonzero relation (the coefficient at zero cannot cancel h≥2h\geq2). The same statement holds on a translated progression.

Taking Q=qnQ=q^n, (5) yields L≥qn(t+1)/2L\geq q^{n(t+1)/2}. The calculation above with H−1H-1 replaced by nlog⁡2q/2n\log_2q/2 gives, when nlog⁡2q≥6n\log_2q\geq6,

η(Bt,L(A))≤4(nlog⁡2q+1)q−n.(6)\eta(B_{t,L}(A))\leq4(n\log_2q+1)q^{-n}. \tag{6}

Thus making Prouhet templates more efficient does not repair full intervals with complete-profile progression focusing. This is not a bound against sparse or nonpointwise lifts.

4. An exact sparse signed-span target

For a finite indexed nonzero vector family C=(ci)C=(c_i), let Σ(C)={∑iϵici:ϵi∈{0,±1}}\Sigma(C)=\{\sum_i\epsilon_ic_i:\epsilon_i\in\{0,\pm1\}\}. Then

∃w≠0: w,2w∈Σ(C)⟺C has a nonzero relation of height at most three.(7)\boxed{\exists w\ne0:\ w,2w\in\Sigma(C) \quad\Longleftrightarrow\quad C\text{ has a nonzero relation of height at most three}.} \tag{7}

If w=ϵ⋅Cw=\epsilon\cdot C and 2w=δ⋅C2w=\delta\cdot C, then 2ϵ−δ2\epsilon-\delta is a nonzero height-three relation. It is nonzero because coordinatewise 2ϵ=δ2\epsilon=\delta would force both to vanish.

Conversely, write a height-three relation zz coordinatewise as z=2ϵ−δz=2\epsilon-\delta, with both vectors ternary. If w=ϵ⋅C≠0w=\epsilon\cdot C\ne0, the desired representations follow. If w=0w=0, either ϵ\epsilon is a nonzero ternary relation, or ϵ=0\epsilon=0 and δ=−z\delta=-z is one. For any nonzero ternary relation ∑isici=0\sum_i s_ic_i=0, choose sj≠0s_j\ne0. Then

w=cj≠0,2w=cj−sj∑i≠jsici∈Σ(C).w=c_j\ne0,\qquad 2w=c_j-s_j\sum_{i\ne j}s_ic_i\in\Sigma(C).

This proves (7). Forcing the signed-span property in some class of every QQ-coloring is therefore exactly a height-three chromatic lower bound, not a weaker route around coefficient height. It still would not by itself prove extraction for a tensor with such a carrier.

The algebraic identities, actual-color quantifiers, extraction bounds, and Vandermonde scope are author-recorded; a separate reviewer checked them, and (7) was checked separately. No computation was used; no extraction-preserving flattening theorem is claimed.