Wiki
Wiki

Research notes on every problem, and a library of the papers behind them. Built from the open erdos repository.

Updated

Heisenberg frame obstruction


Rejected parameterized construction, not a counterexample. The template below has a rigorous independence certificate on one special row. That certificate cannot extend over the extra vertex. No claim of independence control on the entire old vertex set is made.

1. Prescribed full components

Let q≥3q\ge3 be an odd prime power, r=q2r=q^2, and W=Fq2W=\mathbb F_q^2. Choose a nonsquare DD, put

N(x1,x2)=x12−Dx22,Ω(x,y)=x1y2−x2y1,N(x_1,x_2)=x_1^2-Dx_2^2,\qquad \Omega(x,y)=x_1y_2-x_2y_1,

and let BNB_N be the polar bilinear form of NN. For d≠0d\ne0, the linear forms BN(a,d)B_N(a,d) and Ω(a,d)\Omega(a,d) are independent: their determinant is −2N(d)≠0-2N(d)\ne0.

Take vertices (x,z,t)∈W×Fq×Fq(x,z,t)\in W\times\mathbb F_q\times\mathbb F_q, together with ∞\infty, and colors a∈Wa\in W. Prescribe the qq color-aa full components

Qa,b={(x,b+Ω(a,x),N(x−a)):x∈W},b∈Fq.Q_{a,b}=\{(x,b+\Omega(a,x),N(x-a)):x\in W\}, \qquad b\in\mathbb F_q.

Each has order rr. Components in the same color are disjoint. Two prescribed components of different colors meet once: equality of their tt and zz coordinates gives the two independent linear equations just described. Thus their clique edges are compatible.

The transformations

Th,c(x,z,t)=(x+h,z+c+Ω(h,x),t)T_{h,c}(x,z,t)=(x+h,z+c+\Omega(h,x),t)

fix ∞\infty, form a group of order q3q^3, and translate the colors by a↦a+ha\mapsto a+h. They preserve the prescribed components. For t=0t=0, a point belongs to prescribed components in one color; for t≠0t\ne0, it does so in q+1q+1 colors. This uses the norm fiber sizes ∣N−1(0)∣=1|N^{-1}(0)|=1 and ∣N−1(s)∣=q+1|N^{-1}(s)|=q+1 for s≠0s\ne0.

Every unprescribed pair therefore has at least q2−2(q+1)>0q^2-2(q+1)>0 colors whose prescribed components contain neither endpoint. The action has trivial stabilizers on unordered edges: an element fixing an old point is the identity, and a group of odd order cannot interchange the two endpoints of an edge. One may choose a permitted color on each edge orbit and propagate it. Consequently equivariant component-preserving completions exist as colorings. This is a completion statement only, not an independence statement.

2. The frame coloring of the low-incidence row

Put S={(x,z,0)}S=\{(x,z,0)\}, of order q3q^3. In color aa, the qq points with x=ax=a are isolated in SS, since they lie in different prescribed full components. Call them holes.

For every s∈Fq×s\in\mathbb F_q^\times and b∈Fqb\in\mathbb F_q, color the clique

Ra,s,b={(x,b+Ω(a,x),0):N(x−a)=s}R_{a,s,b}=\{(x,b+\Omega(a,x),0):N(x-a)=s\}

with color aa. These are q(q−1)=r−qq(q-1)=r-q cliques of order q+1q+1, partitioning the nonholes in that color. Their edges over all colors partition exactly the pairs in SS with different xx-coordinates. Indeed the equal-norm and equal-intercept equations uniquely determine aa for such a pair, and their common norm is nonzero by anisotropy. Pairs with the same xx-coordinate can be colored equivariantly while avoiding the hole color xx.

Each resulting color graph on SS has independence exactly rr. The clique partition and holes give the upper bound. To attain it, take all holes. For each s≠0s\ne0, select one vertex from each of its qq blocks with distinct xx-coordinates, using a matching from the qq block labels into the q+1q+1 points of the norm circle. Different norm circles use different coordinates. Thus the selected vertices also avoid all additional same-coordinate edges.

3. Robustness defeats the extra vertex

Deleting any qq nonhole vertices from SS still leaves an independent rr-set in every specified color aa. In a fixed norm circle, the preceding matching problem is Kq,q+1K_{q,q+1} with some cells deleted. A Hall obstruction on kk left vertices requires at least

k(q+2−k)≥q+1(1≤k≤q)k(q+2-k)\ge q+1\qquad(1\le k\le q)

deleted cells. At most qq deletions in total cannot create one. Make the matchings separately for all norm circles and retain all holes.

Equivariance forces ∞\infty to have exactly qq neighbors of each color in SS: the action is transitive on SS, on the q2q^2 colors, and has color kernel the central zz-translations. Those neighbors are nonholes by component preservation. The robust independent rr-set can avoid them, and adjoining ∞\infty gives an independent (r+1)(r+1)-set.

Thus this particular frame completion is rigorously excluded. A successful modification would need a low-row color graph with a qq-vertex nonhole set meeting every maximum independent set; the frame graph has no such set. No simultaneous replacement, or whole-graph independence certificate, was obtained.

4. Every clique-component certificate fails when q is prime

For odd prime qq, there is a broader obstruction. No equivariant component-preserving completion can satisfy the desired independence bounds if each color graph restricted to SS is a disjoint union of cliques. This does not assume the norm-frame partition of Section 2.

Equivariance makes all color graphs on SS have the same edge count

e0=(q32)q2=q4−q2.e_0=\frac{\binom{q^3}{2}}{q^2}=\frac{q^4-q}{2}.

Their independence number must equal q2q^2 in any proposed counterexample. It is at most q2q^2 by assumption. If it were at most q2−1q^2-1, deleting the qq isolated holes and using complementary Turan would instead give

e0≥pq2−q−1(q3−q)=e0+2q+1.e_0\ge p_{q^2-q-1}(q^3-q)=e_0+2q+1.

Fix a color. Under the clique-component assumption it has exactly q2−qq^2-q nonhole components. The central group of order qq permutes them in orbits of length one or qq. Thus the number ff of fixed nonhole components is divisible by qq. Every fixed component contains a whole xx-column of qq points. The number of such full columns per color is the same by equivariance and is at most one: each uses (q2)\binom q2 same-coordinate edges, and the q2q^2 colors must share just q2(q2)q^2\binom q2 such edges. Hence f≤1f\le1, and therefore f=0f=0.

Every nonhole component now contains at most one point of any column. Indeed two points in a column differ by a nonidentity central translation. That translation makes the component intersect its image, so stabilizes it. Since qq is prime this would make the component fixed by the entire central group, which was excluded.

The color-neighborhood of ∞\infty in SS is one whole nonhole column. To meet every maximum independent set in a union of cliques, a set must contain some entire component: otherwise choose one vertex outside it from each component. The star column must therefore contain an entire nonhole component, necessarily a singleton. Its central orbit supplies qq additional isolated vertices.

After removing these and the original holes, complementary Turan gives, with n=q3−2qn=q^3-2q and b=q2−2q>0b=q^2-2q>0,

2e0≥2pb(n)≥n2b−n.2e_0\ge2p_b(n)\ge\frac{n^2}{b}-n.

But direct subtraction yields

n2b−n−(q4−q)=q3+3q+4qq−2>0,\frac{n^2}{b}-n-(q^4-q) =q^3+3q+\frac{4q}{q-2}>0,

a contradiction. Thus, at least for prime qq, replacing the frame by another clique partition cannot produce the missing low-row certificate. Non-clique color components remain a possible direction, with no established global independence certificate.

The Hall obstruction and this broader prime-order argument were checked independently. No finite search was used.