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Vesztergombi: On large distances in planar sets

Full paper in Markdown.


Full paper in Markdown.

Katalin Vesztergombi, "On large distances in planar sets," Discrete Mathematics, 67(2), 191-198, 1987. https://doi.org/10.1016/0012-365x(87)90027-6

Overview

For a finite set S⊂R2S\subset\mathbb R^2 of nn points, let d1>d2d_1>d_2 be its two largest distinct interpoint distances, and let nin_i count unordered pairs at distance did_i. The paper proves the sharp bound

n2≤32n.n_2\le \frac32 n.

This is the unnumbered main theorem stated on p. 192 and completed on p. 197. The introductory Theorem A, n1≤nn_1\le n, is explicitly attributed to Hopf–Pannwitz and Sutherland and is therefore cited background, not a new result (p. 191). Likewise, Theorem B, n2≤43nn_2\le \frac43n when SS consists of the vertices of a convex polygon, is quoted from the author's earlier paper [3] (p. 191).

Pairs at distance d1d_1 and d2d_2 are colored red and blue, respectively, and points are classified as outer or inner according to whether they lie on the boundary of conv⁡S\operatorname{conv}S. Proposition 1 says that every red edge joins two outer points, while Proposition 2 excludes the four-vertex configuration called a forbidden NN: two consecutive blue edges followed by a red edge among suitably ordered outer points (p. 191). Proposition 3 shows that every blue edge has at least one outer endpoint, and Proposition 4 restricts the other blue incidences of an inner point lying in a separating fan of blue edges from an outer point (p. 192).

The proof proceeds by induction after deleting vertices of blue degree 00 or 11. It then analyzes an inner point with at least three blue neighbors. Three geometric cases for a chosen triple of outer neighbors are considered on pp. 192–194. In the first two cases the geometry forces a deletable degree-11 vertex; the third case is impossible because it would make two circles have three common points. Consequently, in the reduced configuration every inner point has blue degree exactly 22 (p. 194).

For an outer point uu, an outer blue neighbor vv such that uu has blue neighbors on both sides of the line uvuv is called a middle neighbor, and the corresponding oriented incidence is a middle edge (pp. 194–195). Proposition 5 forbids inner blue edges at the middle neighbors of an outer vertex of outer blue degree at least 33 (p. 195). Proposition 6 bounds the inner blue degree of an outer vertex of outer blue degree 33 by 11 (p. 195). Proposition 7 eliminates inner blue edges at vertices of outer degree 44 after the inductive reductions (pp. 195–196), and Proposition 8 shows that outer blue degree cannot exceed 44 (p. 196).

The final count uses a directed graph GG on the outer points whose arcs are the middle edges directed away from their defining vertex (pp. 196–197). Its components are isolated vertices, paths, and circuits; vertices on nontrivial components alternate between tightly constrained outer degrees. If m1,m2,m3m_1,m_2,m_3 count, respectively, isolated vertices, vertices on circuits, and vertices on paths, and if kk is the number of path components, then the number p1p_1 of outer points is

p1=m1+m2+m3.p_1=m_1+m_2+m_3.

Writing q1q_1 for the number of outer blue edges and q2q_2 for the number of blue edges incident with inner points, the displayed estimates on p. 197 are

q1≤12(2m1+3m2+3m3−k),q2≤2m1+2k.q_1\le \frac12(2m_1+3m_2+3m_3-k),\qquad q_2\le 2m_1+2k.

Since every inner point has blue degree 22, the number p2p_2 of inner points satisfies p2=q2/2≤m1+kp_2=q_2/2\le m_1+k. Substitution into n2=q1+q2n_2=q_1+q_2 yields n2≤32(p1+p2)=32nn_2\le\frac32(p_1+p_2)=\frac32n (p. 197).

Sharpness is asserted by an explicit construction on pp. 197–198. For n=2mn=2m, take outer points v1,…,vmv_1,\ldots,v_m forming a regular mm-gon and inner points u1,…,umu_1,\ldots,u_m satisfying

d(vi,ui)=d(ui,vi+1)=d2d(v_i,u_i)=d(u_i,v_{i+1})=d_2

with indices modulo mm. Together with the mm occurrences of d2d_2 among the outer vertices, this gives n2=3m=32nn_2=3m=\frac32n. The paper concerns only the multiplicity of the second-largest distance; it gives no general estimates for the third or subsequent distinct distances.

Relation to E132

This source bears on Problem 132.

Put N=∣A∣N=|A|, list the distinct distances determined by AA as

λ1>λ2>λ3>⋯ ,\lambda_1>\lambda_2>\lambda_3>\cdots,

and write

μ(λ)=∣{{x,y}⊂A:∣x−y∣=λ}∣.\mu(\lambda)=\bigl|\{\{x,y\}\subset A:|x-y|=\lambda\}\bigr|.

Then Vesztergombi's did_i is λi\lambda_i and her nin_i is μ(λi)\mu(\lambda_i). The cited Hopf–Pannwitz–Sutherland result (Theorem A, p. 191) gives

μ(λ1)≤N,\mu(\lambda_1)\le N,

so the diameter is one distance of the kind required in E132. The paper's new theorem gives only

μ(λ2)≤32N.\mu(\lambda_2)\le \frac32N.

Thus, if μ(λ2)≤N\mu(\lambda_2)\le N in a particular configuration, the two distances λ1\lambda_1 and λ2\lambda_2 settle the first part of E132 for that configuration. In the remaining regime, the theorem merely narrows the obstruction to

N<μ(λ2)≤32N.N<\mu(\lambda_2)\le\frac32N.

The construction on pp. 197–198 attains the upper endpoint, showing that no universal argument can prove that the second-largest distance itself always has multiplicity at most NN. It is not a counterexample to E132: the paper does not count the multiplicities of λ3,λ4,…\lambda_3,\lambda_4,\ldots and therefore does not show that every distance other than the diameter occurs more than NN times.

The potentially reusable part is the two-layer geometric decomposition. In E132 notation, color pairs at λ1\lambda_1 red and pairs at λ2\lambda_2 blue. Propositions 1–4 (pp. 191–192) control how these two graphs meet the convex hull, while Propositions 5–8 (pp. 195–196) and the middle-edge graph on pp. 196–197 reduce the blue graph to components whose edge counts can be charged to outer and inner vertices. This could enter an E132 argument by first separating the case μ(λ2)≤N\mu(\lambda_2)\le N and then using the structural restrictions forced by μ(λ2)>N\mu(\lambda_2)>N to seek a lower distance λj\lambda_j with μ(λj)≤N\mu(\lambda_j)\le N.

The method does not automatically extend to λj\lambda_j for j≥3j\ge3: several steps use the fact that every distance larger than λ2\lambda_2 must equal the single value λ1\lambda_1. In particular, the deductions behind Propositions 3–4 and the forbidden-NN arguments lose this dichotomy at lower distance levels. The paper therefore proves neither the existence of a second rare distance for every planar set nor that the number of distances of multiplicity at most NN tends to infinity with NN.