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Uniform extraction survives every finite incidence cover of axis lines


Row-projection simplification. Deleting duplicated rows shows that the duplicated-cover family has exactly the same chromatic supremum as ordinary covers, and inherits the stronger bound ρ≥e−π2/2\rho\ge e^{-\pi^2/2} directly. Section 7 remains a valid earlier proof, but its sine-moment construction is unnecessary for row duplication. The new fixed-partial-template obstruction on the same linked page also sharpens Section 8's Ramsey limitation. No unbounded coloring is proved.

Standing and theorem

Let Lt=L(d1,…,dt)L_t=L(d_1,\ldots,d_t) be the full axis-line indicator family on Xt=∏i≤t[di]X_t=\prod_{i\leq t}[d_i], with di≥3d_i\geq3. This page proves that the direct axis-line extraction estimate holds uniformly over all finite bipartite-incidence covers of its point-by-line matrix, not merely over literal boxes or one chosen sequence of twists.

The stronger Section 7 theorem also permits any common row-duplication factor before taking the cover, with one bound ρ≥e−2π2\rho\ge e^{-2\pi^2} independent of every parameter. Both analytic statements and the integer lifting construction are author-recorded; a separate reviewer checked them.

For every cover degree mm, every such covered configuration L~t\widetilde L_t satisfies

ρ(L~t)≥min⁡i≤t∏j=i+1tcos⁡(π/dj)di.(1)\rho(\widetilde L_t)\geq \min_{i\leq t}\prod_{j=i+1}^t\cos(\pi/d_j)^{d_i}. \tag{1}

In particular di=i+2d_i=i+2 gives

ρ(L~t)≥e−π2/2(2)\rho(\widetilde L_t)\geq e^{-\pi^2/2} \tag{2}

independently of t,mt,m, and every choice of incidence permutations. There is one δ>0\delta>0 giving full dissociated extraction from every subset of every one of these covers.

Section 7 also permits any common finite row-duplication factor RR before taking the incidence cover. For di=i+2d_i=i+2, all of these larger families have the uniform real-Sidon bound e−2π2e^{-2\pi^2}, independently of RR, the cover degree, and the permutations. This amplifies column support sizes, while each row still has degree tt.

Separately, every nonzero integer relation of a finite 0/10/1 matrix becomes a nonzero ternary relation in a suitable finite incidence cover. For an axis-line relation of coefficient height hh, cover degree at most h⌊t/2⌋h\lfloor t/2\rfloor suffices.

Neither statement controls an arbitrary coloring of the cover. In particular, it is not proved that some cover must have dissociated chromatic number comparable to the rational coloring number of its base. That would be a sufficient new route, not a consequence established here.

1. Exact meaning of a finite incidence cover

Let A∈{0,1}X×VA\in\{0,1\}^{X\times V} be a finite matrix. For each incidence Ax,v=1A_{x,v}=1, choose a permutation πx,v\pi_{x,v} of [m][m]. The degree-mm covered matrix has row labels (x,a)∈X×[m](x,a)\in X\times[m], column labels (v,b)∈V×[m](v,b)\in V\times[m], and

A~(x,a),(v,b)={1,Ax,v=1 and a=πx,v(b),0,otherwise.(3)\widetilde A_{(x,a),(v,b)} = \begin{cases} 1,& A_{x,v}=1\ \text{and }a=\pi_{x,v}(b),\\ 0,&\text{otherwise}. \end{cases} \tag{3}

This is precisely a covering of the bipartite incidence graph that preserves its row and column types. The permutations are independent choices for different base incidences; connectivity is not required.

Every covered column has the same support size as its base column. Every covered row has the same degree as its base row. If the base columns are distinct and nonzero, so are the covered columns: their projections to base row supports distinguish different base columns, and different lifts of one base column have disjoint nonempty supports. In particular covers of LtL_t are genuine sets of distinct nonzero 0/10/1 vectors, without antipodal pairs.

2. Every axis-line cover has the twisted-layer decomposition

Write Xt=Xt−1×[d]X_t=X_{t-1}\times[d], d=dtd=d_t. Split covered rows into the dd sets

{(x,s,a):x∈Xt−1, a∈[m]},s∈[d].\{(x,s,a):x\in X_{t-1},\,a\in[m]\}, \qquad s\in[d].

The old directions i<ti<t in each layer form an arbitrary degree-mm cover of Lt−1L_{t-1}. These dd covers need not be isomorphic; the uniform induction applies separately to each one.

The new direction has base columns indexed by x∈Xt−1x\in X_{t-1}. For its lift labeled (x,b)(x,b), the row in layer ss is

(x,s,π(x,s), ℓx(b)).(x,s,\pi_{(x,s),\,\ell_x}(b)).

For each ss, define the bijection of the covered old row set

Ts(x,b)=(x,π(x,s), ℓx(b)).(4)T_s(x,b)=(x,\pi_{(x,s),\,\ell_x}(b)). \tag{4}

Thus the new columns are exactly the disjoint transversals

ny=∑s=1de(Tsy,s),y∈Xt−1×[m].(5)n_y=\sum_{s=1}^d e_{(T_s y,s)}, \qquad y\in X_{t-1}\times[m]. \tag{5}

An old column lies wholly in one layer and meets each new transversal in at most one point. This decomposition used no restriction on the permutations in (3), and therefore covers every finite incidence cover.

3. Uniform directional Sidon induction over all covers

Put ad=cos⁡(π/d)a_d=\cos(\pi/d). The elementary root-polygon lemma states: for every u∈Tu\in\mathbb T, there is a finite random Y∈TY\in\mathbb T with

Yd=u,EY=ad.(6)Y^d=u,\qquad \mathbb EY=a_d. \tag{6}

The expectation is target-independent, because the convex hull of the dd-th roots of uu contains the disk of radius ada_d.

We prove simultaneously for all degree-mm covers that a polynomial with total coefficient magnitude WiW_i in direction ii obeys

max⁡Re⁡P≥∑i≤tri,tWi,ri,t=∏j=i+1tadjdi.(7)\max\operatorname{Re}P\geq \sum_{i\leq t}r_{i,t}W_i,\qquad r_{i,t}=\prod_{j=i+1}^t a_{d_j}^{d_i}. \tag{7}

For t=1t=1, all mm covered lines have disjoint supports, so their characters can be prescribed independently and r1,1=1r_{1,1}=1.

At the induction step, decompose PP into old layer polynomials and new terms

∑yby∏s=1dzTsy,s.(8)\sum_y b_y\prod_{s=1}^d z_{T_s y,s}. \tag{8}

In every old layer, first multiply every direction-ii coefficient by addia_d^{d_i}. Choose its phases by (7) for that layer's own covered matrix, then hold all those phase choices fixed.

For each new transversal label yy, prescribe uyu_y so that multiplying its dd point phases by a common dd-th root of uyu_y makes its term equal to ∣by∣|b_y|. If by=0b_y=0, choose any target. Choose independent YyY_y as in (6), and make the replacement

zTsy,s′=zTsy,sYyfor every y,s.(9)z'_{T_s y,s}=z_{T_s y,s}Y_y \quad\text{for every }y,s. \tag{9}

Because TsT_s is a bijection, this assigns each row phase exactly once. Each new term is aligned deterministically. Each old direction-ii column uses did_i distinct transversal labels, so its expected multiplier is exactly addia_d^{d_i}. Thus the expected old polynomial is precisely the rescaled polynomial optimized earlier. Its directional bound is ri,t−1addiWir_{i,t-1}a_d^{d_i}W_i, while the new terms contribute WtW_t. A finite random outcome attains the expectation. This proves (7) and (1).

The proof uses neither identical old covers in the different layers nor independence between layers. It requires independence only across transversal labels. This is why arbitrary incidence permutations do not change the estimate.

For di=i+2d_i=i+2, the already proved elementary inequality

−log⁡cos⁡(π/n)≤π22n(n−1),n≥4,-\log\cos(\pi/n)\leq\frac{\pi^2}{2n(n-1)},\qquad n\geq4,

telescopes to ri,t≥e−π2/2r_{i,t}\geq e^{-\pi^2/2}, giving (2). More generally, the same uniform result holds whenever sup⁡idi∑j>idj−2<∞\sup_i d_i\sum_{j>i}d_j^{-2}<\infty, with the constant recorded in the axis-line extraction theorem.

4. One extraction constant for every covered matrix

There are countably many finite covers in question: for each t,mt,m there are finitely many choices of the permutations (3). Place one copy of each covered configuration in its own free-abelian direct summand. Let Λ\Lambda be their union in the resulting countable direct sum.

Every finite polynomial on Λ\Lambda splits between finitely many summands. Their phase choices are independent, so (2) gives the same positive-real Sidon estimate on the whole union. Pisier's Theorem 2, already checked in the supplied full source, applies once to this one Sidon set. It supplies one full-dissociation extraction constant δ>0\delta>0 for every finite subset of Λ\Lambda, hence uniformly for all t,mt,m and incidence covers.

No quantitative dependence of δ\delta on (2) is asserted. The direct sum is used only to make uniformity across unrelated covers explicit; compatible covering maps or nested choices of permutations are unnecessary.

5. Every integer relation has a ternary covering lift

Let AA have nonzero 0/10/1 columns, and let

0≠a=(av)v∈V∈ker⁡ZA.(10)0\ne a=(a_v)_{v\in V}\in\ker_{\mathbb Z}A. \tag{10}

For each base row xx, set

px=∑v:Ax,v=1av>0av=∑v:Ax,v=1av<0∣av∣.(11)p_x=\sum_{\substack{v:A_{x,v}=1\\a_v>0}}a_v =\sum_{\substack{v:A_{x,v}=1\\a_v<0}}|a_v|. \tag{11}

Set m=max⁡xpxm=\max_x p_x. This is positive. Also ∣av∣≤m|a_v|\leq m for every vv, since every column is nonzero and (11) holds at a row in its support.

Select copies 1,…,∣av∣1,\ldots,|a_v| of each column vv and give them the common sign sgn⁡(av)\operatorname{sgn}(a_v). At a row xx, its selected positive incidences and selected negative incidences both number pxp_x. Pair them bijectively and give the pairs distinct labels from [m][m]. Define πx,v\pi_{x,v} on each selected column copy to send it to its pair's label.

For each fixed (x,v)(x,v), distinct selected copies receive distinct row labels, so this partial injection extends to a permutation of [m][m]. Choose arbitrary extensions, independently for all incidences. In the covered matrix, every used row receives exactly one selected positive incidence and one selected negative incidence; unused rows receive none. Therefore

∑v:av≠0sgn⁡(av)∑b=1∣av∣A~v,b=0(12)\sum_{v:a_v\ne0}\operatorname{sgn}(a_v) \sum_{b=1}^{|a_v|}\widetilde A_{v,b}=0 \tag{12}

is a nonzero ternary relation on distinct column labels. For bases with distinct nonzero columns, including axis lines, these are also distinct actual vectors, as checked in Section 1.

If ∣av∣≤h|a_v|\leq h and every base row has degree at most Δ\Delta, then

m≤h⌊Δ/2⌋.(13)m\leq h\lfloor\Delta/2\rfloor. \tag{13}

Indeed the positive and negative incident base columns are disjoint sets, and (11) is at most hh times the cardinality of either set. Their smaller cardinality is at most ⌊Δ/2⌋\lfloor\Delta/2\rfloor. For LtL_t, Δ=t\Delta=t, proving the asserted degree bound.

This is an existence construction for a cover tailored to one integer relation. It does not say that an arbitrary fixed cover lifts that relation, or that arbitrary colors of the selected copies agree.

6. Exact missing color statement

For a finite base AA, let

Γ(A)=sup⁡A~ a finite incidence coverχ1(A~).\Gamma(A)=\sup_{\widetilde A\text{ a finite incidence cover}} \chi_1(\widetilde A).

No general lower bound

Γ(A)≥χQ(A)or evenΓ(A)≥∣V(A)∣/∣X(A)∣(14)\Gamma(A)\geq\chi_{\mathbb Q}(A) \quad\text{or even}\quad \Gamma(A)\geq |V(A)|/|X(A)| \tag{14}

has been established here. Either displayed bound, applied to the linear axis-line bases, would give unbounded covered dissociated coloring because

∣Lt∣∣Xt∣=∑i≤t1i+2⟶∞.\frac{|L_t|}{|X_t|} =\sum_{i\leq t}\frac1{i+2}\longrightarrow\infty.

Together with the uniform extraction theorem, that would complete the finite-block obligation. Equation (14) is only a proposed sufficient theorem and is not asserted true.

Section 5 handles a monochromatic relation only when the selected lifted columns happen to share an actual color. A coloring may use different colors at different copies of the same base column. Building one cover for each base relation, or taking their disjoint union, does not remove that freedom. Covers can also have relations whose signed fiber totals are all zero, so projection to base relations is not a full description of their relation systems.

Thus the remaining problem is a genuine color-unavoidable covering construction, not integer coefficient flattening alone. No computation or external covering/Ramsey theorem is used in this page.

7. Uniform row duplication also preserves covered extraction

For a fixed integer R≥1R\geq1, replace each row xx of the axis-line matrix by rows (x,r)(x,r), r∈[R]r\in[R], with identical entries. Denote this matrix by At[R]A_t^{[R]}. It has exactly the same integer and rational relation lattices as AtA_t. Now take an arbitrary degree-mm incidence cover of At[R]A_t^{[R]}, with independent permutations for all incidences at these duplicated rows.

Theorem. For di=i+2d_i=i+2, every such covered matrix has

ρ(A~t[R])≥e−2π2,(15)\rho\bigl(\widetilde A_t^{[R]}\bigr) \geq e^{-2\pi^2}, \tag{15}

uniformly in t,R,mt,R,m and all incidence permutations. The whole collection consequently has one proportional full-dissociation extraction constant.

The proof needs controlled moments up to RR, because an old column can now meet a new column in as many as RR points. No chromatic amplification follows merely from allowing these extra incidences.

7.1 A finite root distribution with several target-independent moments

Let D=RdD=Rd, where R≥1R\geq1 and d≥4d\geq4, and put

L=D−R−1,αj=sin⁡(j+1)πL+2(0≤j≤L),Q=∑j=0Lαj2.L=D-R-1,\qquad \alpha_j=\sin\frac{(j+1)\pi}{L+2}\quad(0\leq j\leq L), \qquad Q=\sum_{j=0}^L\alpha_j^2.

For any u∈Tu\in\mathbb T, give a DD-th root yy of uu probability

P(Y=y)=1DQ∣∑j=0Lαjyj∣2.(16)\mathbb P(Y=y) =\frac1{DQ}\left|\sum_{j=0}^L\alpha_jy^j\right|^2. \tag{16}

These weights are nonnegative and sum to one. Indeed the polynomial inside (16), after taking absolute square, has Laurent degree at most L<DL<D; averaging on the DD-th roots annihilates every nonconstant Laurent monomial appearing in it. The remaining coefficient is QQ.

Similarly, for 0≤k≤R0\leq k\leq R,

YD=u,EYk=ck:=∑j=0L−kαjαj+kQ.(17)Y^D=u,\qquad \mathbb EY^k=c_k:= \frac{\sum_{j=0}^{L-k}\alpha_j\alpha_{j+k}}{Q}. \tag{17}

There are no aliases: after multiplication by yky^k, all exponents lie strictly between −D-D and DD, since L+R=D−1L+R=D-1. Thus (17) is independent of the prescribed target uu. In particular c0=1c_0=1, and ck>0c_k>0 for 1≤k≤R1\leq k\leq R.

Extend the vector α\alpha by zero to Z\mathbb Z, and let SS be the shift operator on its square-summable coordinate space. The sine eigenvector identity gives

c1=cos⁡πL+2,∥(S−I)α∥22=2Q(1−c1).c_1=\cos\frac{\pi}{L+2},\qquad \|(S-I)\alpha\|_2^2=2Q(1-c_1).

Using Sk−I=∑a=0k−1Sa(S−I)S^k-I=\sum_{a=0}^{k-1}S^a(S-I) and the triangle inequality,

1−ck=∥(Sk−I)α∥222Q≤k2(1−c1)≤π2k22(D−R+1)2.(18)1-c_k =\frac{\|(S^k-I)\alpha\|_2^2}{2Q} \leq k^2(1-c_1) \leq\frac{\pi^2k^2}{2(D-R+1)^2}. \tag{18}

For k≤R,d≥4k\leq R,d\geq4, the last upper bound is less than 5/95/9, because π2<10\pi^2<10 and D−R+1≥3R+1D-R+1\geq3R+1. Hence −log⁡ck≤−log⁡(1−v)≤v/(1−v)≤9v/4-\log c_k\leq-\log(1-v)\leq v/(1-v)\leq9v/4, with vv equal to that bound in (18). As D−R+1≥3D/4D-R+1\geq3D/4, this proves

ck≥exp⁡(− 2π2k2D2)(0≤k≤R).(19)c_k\geq \exp\left(-\,\frac{2\pi^2k^2}{D^2}\right) \quad(0\leq k\leq R). \tag{19}

All distributions are finite. Their probabilities may depend on uu; the moments used in the induction do not.

7.2 Geometry of a covered duplicated-row extension

Split the covered rows according to the last base coordinate s∈[d]s\in[d], d=dtd=d_t. The old directions in each layer form an arbitrary degree-mm cover of At−1[R]A_{t-1}^{[R]}.

The new-axis columns form a partition of all covered rows, each block having exactly D=RdD=Rd points. A new block has a fixed base point x∈Xt−1x\in X_{t-1}. An old direction-ii column lies in one layer and projects onto did_i distinct old base points, with RR covered rows over each one. Therefore its intersections with the new blocks have sizes k1,k2,…k_1,k_2,\ldots satisfying

0≤ka≤R,∑aka=Rdi,∑aka2≤R2di.(20)0\leq k_a\leq R,\qquad \sum_a k_a=Rd_i,\qquad \sum_a k_a^2\leq R^2d_i. \tag{20}

The upper bound RR uses preservation of base point labels in an incidence cover. It is not claimed for arbitrary unstructured block partitions of the same total size.

7.3 Prescaled induction

For each old covered column ℓ\ell, define its fixed multiplier

γℓ=∏acka,\gamma_\ell=\prod_a c_{k_a},

using its actual intersection sizes in (20). By (19),

γℓ≥exp⁡(− 2π2didt2)if ℓ has direction i<t.(21)\gamma_\ell\geq \exp\left(-\,\frac{2\pi^2d_i}{d_t^2}\right) \quad\text{if }\ell\text{ has direction }i<t. \tag{21}

These multipliers may depend on the incidence permutations and the column, but do not depend on phase targets.

Multiply every old coefficient by its γℓ\gamma_\ell, optimize the resulting polynomial in each old layer, and then fix those phases. For each new block prescribe uu to align its coefficient. Independently choose its YY from (16), and multiply every row phase in that block by YY. Every new term is exactly aligned because the block has DD points and YD=uY^D=u. An old column has expected multiplier exactly γℓ\gamma_\ell, by independence across new blocks and (17). Thus expectation recovers precisely the prescaled old polynomial.

The resulting directional lower bound is

max⁡Re⁡P≥∑i≤texp⁡(−2π2di∑j=i+1tdj−2)Wi.(22)\max\operatorname{Re}P \geq\sum_{i\leq t} \exp\left(-2\pi^2d_i\sum_{j=i+1}^t d_j^{-2}\right)W_i. \tag{22}

At t=1t=1, the covered columns have disjoint supports even after row duplication, so the induction starts with parameter one. All later sides satisfy dt=t+2≥4d_t=t+2\geq4, as required in (16)--(19). Finally

di∑j>idj−2≤1d_i\sum_{j>i}d_j^{-2}\leq1

for di=i+2d_i=i+2. This proves (15).

For the uniform extraction assertion, enlarge the direct sum in Section 4 to include all positive integers RR as well. The collection is still countable, and (15) gives one Sidon estimate on its union. One application of Pisier's theorem supplies one extraction constant for the entire enlarged collection. No finite-stage or duplication-dependent sequence of extraction constants is used.

7.4 Exact chromatic standing of this enlargement

Duplicating rows leaves the base rational coloring number unchanged, but arbitrary covers of the duplicated matrix can have new relation supports. A possible sufficient statement would now be

sup⁡R≥1A~ a finite cover of A[R]χ1(A~)≥χQ(A).(23)\sup_{\substack{R\geq1\\ \widetilde A\text{ a finite cover of }A^{[R]}}} \chi_1(\widetilde A)\geq\chi_{\mathbb Q}(A). \tag{23}

Equation (23) is unproved and not asserted true. Allowing RR provides arbitrarily many incidence positions in each column; it does not increase the number of columns incident to one row, and it does not by itself force selected covering copies to share a color.

The ordinary-cover and row-duplication estimates, and the integer flattening construction, are the proved outcomes. No color-unavoidable covering or sparse-gadget amplification theorem is claimed.

8. Scope of the checked Ramsey input

The digest and relevant full passages of Nešetřil–Rödl–Sales were consulted during research. Theorem 3.2 supplies an ordered partial-Steiner Ramsey host, not a degree-preserving incidence cover. Its fixed-order application does not provide full dissociation or an implementation by the operations above. No new positive result here depends on importing that missing implementation.

A specific full-cover focusing proposal has a precise limitation. An incidence-preserving embedding over a fixed base of a complete finite cover into another cover has image a union of connected components: the embedded vertices already use every allowed incidence port, so no adjacent vertex can lie outside the image. For a connected nontrivial cover (cover degree greater than one), two colors can split one column fiber in each host component isomorphic to it. No embedded copy of that full cover is then fiber-monochromatic.

This does not exclude Ramsey constructions for partial balanced supports, whose row ports need not be exhausted. It also supplies no negative conclusion about the row-duplication enlargement in Section 7. The surviving obligation is still a prechosen finite cover defeating every coloring, rather than a cover chosen after seeing a relation or its colors.