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Near-minimal distance counts on constant-width boundaries


The inverse statement

Theorem. Fix L≥0L\ge0. There is cL>0c_L>0 such that, for all sufficiently large mm, every mm-point subset CC of the boundary of a planar constant-width body with

q(C)≤m/2+Lq(C)\le m/2+L

contains at least cLmc_Lm concyclic points.

This is a restricted inverse theorem. A general convex polygon need not lie on a constant-width boundary. Neither unrestricted assertion of Problem 132 follows from it.

1. Diameter degree and the ranks in a row

Write DD for the body's width, q=q(C)q=q(C), and label the points p0,…,pm−1p_0,\ldots,p_{m-1} counterclockwise. Indices are taken modulo mm. The boundary theorem supplies strict convexity, monotonicity of distance along each directed boundary arc up to the DD-farthest arc, and q≥⌊m/2⌋q\ge\lfloor m/2\rfloor.

We use Altman's maximal-side lemma: a convex vv-gon having a side which attains its diameter determines at least v−2v-2 distances. This is Lemma 1 in the supplied Fishburn paper, whose statement and definition of a maximal side were checked.

If ∣pi−pi+s∣=D|p_i-p_{i+s}|=D, apply that lemma to the two subpolygons having this chord as a side. They have s+1s+1 and m−s+1m-s+1 vertices, so

q≥max⁡{s,m−s}−1.q\ge\max\{s,m-s\}-1.

For a two-vertex subpolygon the needed inequality is trivial. Thus every DD-neighbor of pip_i has index displacement in [m−q−1,q+1][m-q-1,q+1]. In particular its DD-degree aia_i satisfies

ai≤2q−m+3≤2L+3.(1)a_i\le2q-m+3\le2L+3. \tag{1}

List the occurring distances increasingly as d1<⋯<dqd_1<\cdots<d_q. The two strictly increasing directed lists from any pip_i contain each subdiametral distance at most once each. If DD is absent from CC, their total number of missing entries from this palette is 2q−(m−1)≤2L+12q-(m-1)\le2L+1. If DD is present, remove it from the palette. The missing-entry count becomes

2(q−1)−(m−1−ai)≤4L+2.(2)2(q-1)-(m-1-a_i)\le4L+2. \tag{2}

Set E=⌈4L+4⌉E=\lceil4L+4\rceil. Each of the two increasing lists therefore has at least ⌊m/2⌋−1−E\lfloor m/2\rfloor-1-E entries. For sufficiently large mm, the first F=⌊m/3⌋F=\lfloor m/3\rfloor successors of every pip_i lie on its increasing arc, and

∣pi−pi+k∣=dk+ei(k),1≤k≤F,(3)|p_i-p_{i+k}|=d_{k+e_i(k)},\qquad 1\le k\le F, \tag{3}

where ei(k)e_i(k) is nondecreasing and takes integer values in {0,…,E}\{0,\ldots,E\}. It counts omitted palette entries before the kk-th entry. Each row eie_i has at most EE jumps.

2. Four compatible rows

Use the finite van der Waerden theorem to choose NN such that every (E+1)2(E+1)^2-coloring of {0,…,N−1}\{0,\ldots,N-1\} has a monochromatic four-term arithmetic progression. Choose an integer M≥8N(E+1)M\ge8N(E+1). All these constants depend only on LL.

Partition {1,…,F}\{1,\ldots,F\} into MM consecutive intervals of nearly equal length. A row is nonconstant on at most EE of them. Some interval J=[u,v]J=[u,v], of length ΩL(m)\Omega_L(m), therefore has fewer than m/(8N)m/(8N) nonconstant rows.

For sufficiently large mm, all MM intervals

[Na,Na+1],0≤a<M,[N^a,N^{a+1}],\qquad 0\le a<M,

lie in [1,F][1,F]. Each jump is internal to at most one such interval. Some H=[h,Nh]H=[h,Nh] again has fewer than m/(8N)m/(8N) nonconstant rows. Here h≤NM−1h\le N^{M-1} is bounded in terms of LL, independently of mm.

Call a row good if it is constant on both JJ and HH, and color it by its two constant values. Fewer than m/(4N)m/(4N) rows are bad. A bad row spoils at most NN cyclic chains

i,i+h,…,i+(N−1)h.i,i+h,\ldots,i+(N-1)h.

Hence some such chain is all good. Its indices are distinct for sufficiently large mm. Van der Waerden's theorem now supplies four same-colored rows

a,a+k,a+2k,a+3k,a,a+k,a+2k,a+3k,

where k=dhk=dh, 1≤d≤(N−1)/31\le d\le(N-1)/3. In particular k,2k∈Hk,2k\in H and k=OL(1)k=O_L(1).

3. A rotation propagates across a long interval

Put xℓ=pa+ℓkx_\ell=p_{a+\ell k} for 0≤ℓ≤30\le\ell\le3. Their common color on HH and (3) imply

∣x0x1∣=∣x1x2∣=∣x2x3∣,∣x0x2∣=∣x1x3∣.|x_0x_1|=|x_1x_2|=|x_2x_3|, \qquad |x_0x_2|=|x_1x_3|.

They occur in convex cyclic order. The successive triangles are congruent with the same orientation, so an orientation-preserving isometry TT sends x0,x1,x2x_0,x_1,x_2 to x1,x2,x3x_1,x_2,x_3. It is not a translation, since the first three points are noncollinear. Thus TT is a nontrivial rotation.

Let bb be the common row value on JJ and put zj=pa+jz_j=p_{a+j}. For u+2k≤j≤vu+2k\le j\le v and ℓ=0,1,2\ell=0,1,2, (3) gives

∣zj+k−xℓ+1∣=dj−ℓk+b=∣zj−xℓ∣.|z_{j+k}-x_{\ell+1}| =d_{j-\ell k+b} =|z_j-x_\ell|.

The point TzjTz_j has the same three distances to the noncollinear anchors x1,x2,x3x_1,x_2,x_3, so uniqueness of intersection with three prescribed-radius circles gives

zj+k=Tzj.(4)z_{j+k}=Tz_j. \tag{4}

An interval of ΩL(m)\Omega_L(m) vertices is therefore partitioned, by index modulo kk, into at most k=OL(1)k=O_L(1) rotation orbits. Each nonsingleton orbit lies on a positive-radius circle. The largest orbit has ΩL(m)\Omega_L(m) vertices, proving the theorem.

Consequence: boundedly many diameter-inactive points

Corollary. Fix t≥0t\ge0. Along any sequence of nn-point sets in which at most tt points are not incident with a diameter pair, R(A)→∞R(A)\to\infty as n→∞n\to\infty.

Suppose otherwise that R(A)≤KR(A)\le K on an unbounded subsequence. Let CC be its m≥n−tm\ge n-t diameter-active points. By constant_width, these lie on a common constant-width boundary. The pair budget gives

q(C)≤q(A)≤n/2+K≤m/2+t/2+K.q(C)\le q(A)\le n/2+K\le m/2+t/2+K.

The theorem supplies a positive fraction of CC, hence of AA, on one circle. The circle-incidence theorem then gives linearly many rare distances, a contradiction.

Checks and remaining gap

The author checked (1)--(4), including zero diameter degrees, the two palette cases, the shared endpoints of the short intervals, cyclic indices, orientation of the anchor isometry, and its propagation by three anchors, together with the combinatorial selection and rotation argument; the argument is author-recorded. The finite van der Waerden theorem and Altman's stated maximal-side lemma are the external inputs.

For a merely positive-fraction subset m=cnm=cn, bounded rarity only gives q(C)≤n/2+O(1)q(C)\le n/2+O(1). Its excess over m/2m/2 can be linear in nn, so the bounded row-error argument does not apply. No proof makes an arbitrary bounded-rarity configuration have only boundedly many diameter-inactive points. This is the unresolved step, not a conclusion of the inverse theorem.