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Color bounds for correlated port attachments


This page preserves an earlier research route and its local standing. The completed threshold proof is in the solution note.

The overlapping-port theorem extends to arbitrary attachment graphs and internal core graphs when the hubs have positive size. The general graph case remains beyond this family.

Scope and conclusion

Partition the vertices into a fixed finite number of disjoint cores QiQ_i, independent hubs XiX_i, and a port graph PP. Assume:

  • each QiQ_i is completely joined to XiX_i;
  • PP is triangle-free;
  • the edges from XiX_i to PP are arbitrary, but all their port endpoints belong to some independent set NiN_i of PP;
  • there are no other edges, in particular no XiXjX_iX_j edges;
  • each ∣Xi∣/n|X_i|/n has a positive limit.

The internal graphs G[Qi]G[Q_i] and the attachment graphs may be arbitrary. Complementary rows and other correlated neighborhoods are allowed. Along any subsequence on which e/n2→qe/n^2\to q and r/n2→ρr/n^2\to\rho, every coloring in which all seven-cycles are rainbow satisfies

q≤max⁡{1/4,ρ/2}.(1)q\le\max\{1/4,\sqrt{\rho/2}\}. \tag{1}

In particular q>1/4q>1/4 forces ρ≥2q2>1/8\rho\ge2q^2>1/8.

The positive hub-size hypothesis cannot simply be dropped: allowing an arbitrary QiQ_i with Xi=∅X_i=\varnothing would include the original unresolved problem.

A local weighted color bound

First consider one branch with δ(G[Q])≥100\delta(G[Q])\ge100 and ∣X∣≥100|X|\ge100. Write ∣Q∣/n→b|Q|/n\to b, ∣X∣/n→x>0|X|/n\to x>0, and

h=lim⁡e(Q)+∣Q∣∣X∣n2.h=\lim \frac{e(Q)+|Q||X|}{n^2}.

Suppose the available port set has at most an+o(n)an+o(n) vertices, and the attachment edge count is wn2+o(n2)wn^2+o(n^2). Then

ρ≥h+w2ax,(2)\rho\ge h+\frac{w^2}{ax}, \tag{2}

with the quotient omitted if w=0w=0.

Core and join colors

The graph Q∨XQ\vee X has two- and three-edge paths between every pair, avoiding any bounded set needed in the following constructions. For two endpoints in QQ, use q−X−q′q-X-q' and q−u−X−q′q-u-X-q' with ququ an internal edge. For QQ--XX endpoints use an internal neighbor of qq, or an internal two-edge path starting at qq. For two endpoints in XX, use a vertex or an edge of QQ. The degree and size bounds allow all auxiliary vertices to be fresh.

Consequently all edges in F=E(Q)∪E(Q,X)F=E(Q)\cup E(Q,X) have distinct colors: use two- and three-paths for disjoint prescribed edges; extend an adjacent pair to a four-path and close it with a three-path.

Fix δ>0\delta>0 and retain only attachment edges whose port endpoint has at least δn\delta n neighbors in XX. Every retained attachment edge conflicts with every edge of FF. For disjoint edges uv∈Fuv\in F and xaxa, orient u∈Qu\in Q. Use a−z−ua-z-u with z∈NX(a)z\in N_X(a) avoiding the prescribed vertices, and a three-path from vv to xx in Q∨XQ\vee X, avoiding the first path and the other marked endpoints. For a shared XX endpoint, a five-path from the port aa to the QQ endpoint is

a,z,q1,q2,y,u,a,z,q_1,q_2,y,u,

where q1q2q_1q_2 is an internal edge of QQ and z,y∈Xz,y\in X are fresh. Thus the retained attachment colors are disjoint from the FF colors.

The attachment colors

A monochromatic collection of retained attachment edges is a matching. For a common port endpoint, close through a three-edge path in QQ; for a common XX endpoint, use a five-path between the port endpoints through fresh X,Q,Q,XX,Q,Q,X vertices.

If two such same-colored edges are aixi,ajxja_ix_i,a_jx_j, then

∣NX(ai)∩NX(aj)∣≤2.|N_X(a_i)\cap N_X(a_j)|\le2.

Otherwise choose a common neighbor uu outside {xi,xj}\{x_i,x_j\} and a fresh internal edge q1q2q_1q_2 of QQ. The cycle

ai,xi,q1,q2,xj,aj,u,aia_i,x_i,q_1,q_2,x_j,a_j,u,a_i

would repeat their color.

There are only Oδ(1)O_\delta(1) edges in a monochromatic retained collection. Indeed, a fixed sufficiently large number kk of its port neighborhoods would have union of size at least kδn−2(k2)>∣X∣k\delta n-2\binom{k}{2}>|X|. Hence, for each retained color,

∑jdX(aj)≤∣X∣+Oδ(1).\sum_j d_X(a_j)\le |X|+O_\delta(1).

Summing this inequality over its attachment colors gives

ratt≥∑a: dX(a)≥δndX(a)2∣X∣+Oδ(1).r_{\rm att}\ge \frac{\sum_{a:\,d_X(a)\ge\delta n}d_X(a)^2} {|X|+O_\delta(1)}.

The discarded squared-degree sum is O(δn3)O(\delta n^3). Also

∑adX(a)2≥(wn2+o(n2))2an+o(n).\sum_a d_X(a)^2 \ge \frac{(wn^2+o(n^2))^2}{an+o(n)}.

Let n→∞n\to\infty, then δ↓0\delta\downarrow0, and add the disjoint core/join palette. This proves (2).

In particular, complementary port neighborhoods can reduce the attachment cost below its edge count. The correct lower bound in this argument is quadratic in the attachment density, not a claim that all attachment edges are rainbow.

Efficiency despite partial attachment density

For R,a>0R,a>0 put

fR(a)={R/2R−a2,a≤R,a,a≥R.f_R(a)= \begin{cases} R/\sqrt{2R-a^2},&a\le\sqrt R,\\ a,&a\ge\sqrt R. \end{cases}

If h,x,w≥0h,x,w\ge0, w≤axw\le ax, and h+w2/(ax)≤Rh+w^2/(ax)\le R, then

h+w2h+x2≤fR(a).(3)\frac{h+w}{\sqrt{2h+x^2}}\le f_R(a). \tag{3}

Boundary cases with zero denominators are interpreted by limits.

Here is a check of the interior optimization, where reducing attachment density might otherwise seem advantageous. First impose equality in the resource constraint and write

0≤h≤R,x≥(R−h)/a,w=ax(R−h).0\le h\le R,\qquad x\ge(R-h)/a,\qquad w=\sqrt{ax(R-h)}.

The objective tends uniformly to zero as x→∞x\to\infty. The boundaries h=0h=0 and w=0w=0 give at most aa and R/2\sqrt{R/2}. On w=axw=ax, the objective is

R2R−2ax+x2,0≤x≤R/a,\frac R{\sqrt{2R-2ax+x^2}},\qquad 0\le x\le R/a,

whose maximum is fR(a)f_R(a).

There is no interior maximum with 0<w<ax0<w<ax. Put t=2h+x2t=\sqrt{2h+x^2} and β=(h+w)/t\beta=(h+w)/t. The Lagrange equations, with multiplier rescaled by tt, are

1−β/t=μ,βx/t=μw2/(ax2),1=μ 2w/(ax).1-\beta/t=\mu,\qquad \beta x/t=\mu w^2/(ax^2),\qquad 1=\mu\,2w/(ax).

The last equation gives μ>1/2\mu>1/2. The other equations imply

w=2βx2/t,β/t=h/(2h−x2)>1/2,w=2\beta x^2/t,\qquad \beta/t=h/(2h-x^2)>1/2,

contradicting the first. This proves the equality case. Finally fR(a)f_R(a) is nondecreasing in RR, giving (3) for resource at most RR.

For a branch, h≤b2/2+bxh\le b^2/2+bx, so 2h+x2≤b+x\sqrt{2h+x^2}\le b+x. Equations (2)--(3) therefore give

h+w≤fρ(a)(b+x).(4)h+w\le f_\rho(a)(b+x). \tag{4}

This is the same efficiency estimate as in the full-density port theorem, despite arbitrary attachment correlations.

Pruning arbitrary cores

Inside each original QiQ_i, repeatedly remove a vertex of current internal degree below 100100, deleting its remaining internal edges. Across all cores this deletes fewer than 100n100n edges.

Move the removed vertices RiR_i into the port graph. Their only remaining edges are the complete join to XiX_i. For a surviving core, its new attachment set is Ni∪RiN_i\cup R_i, which is independent. If the core empties, absorb XiX_i into the port graph too: its neighborhood is contained in the independent set Ni∪RiN_i\cup R_i. Different XiX_i's have no edges between them, so these absorptions preserve triangle-freeness. Every remaining core has minimum internal degree at least 100100. The hypotheses needed for (2) now hold.

A surviving core of sublinear size causes no problem: the bounded path constructions still exist, while its normalized internal and join contribution may be zero. The positive-linear hub assumption continues to hold for every surviving branch.

The final port calculation

Let AA be the limiting mass of the enlarged port graph, and let α\alpha be a subsequential limit of its maximum independent-set mass. Set a=max⁡{α,A/2}a=\max\{\alpha,A/2\}. The weighted triangle-free estimate proved in the overlapping-port note gives

e(P)/n2≤a(A−a)+o(1).e(P)/n^2\le a(A-a)+o(1).

Every available attachment set has mass at most aa. Sum (4), using ∑i(bi+xi)=1−A\sum_i(b_i+x_i)=1-A, to get

q≤(1−A)fρ(a)+a(A−a)≤(1−a)fρ(a)≤max⁡{1/4,ρ/2}.q\le(1-A)f_\rho(a)+a(A-a) \le(1-a)f_\rho(a) \le\max\{1/4,\sqrt{\rho/2}\}.

The last two inequalities are the already proved endpoint calculation for fRf_R, using A≥aA\ge a and fR(a)≥af_R(a)\ge a. The O(n)O(n) deleted edges do not change qq. If ρ>1/2\rho>1/2, (1) is already trivial from q≤1/2q\le1/2; thus no endpoint-range issue arises.

No assertion is made for arbitrary incomplete core--hub joins, or for directly interconnected hubs. The latter, under different random-template assumptions, are treated in private core hubs. At q=1/4q=1/4, inequality (1) alone gives no lower bound on ρ\rho; handling vanishing density surplus would require an additional stability argument.