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Short-distance spectra under bounded rarity


This is a local necessary condition, not a solution of Problem 132. Write rsr_s for the ss-th smallest positive distance, and assume R(A)≤KR(A)\le K.

A bounded local spectrum

For an absolute constant CC,

#{r∈D(A):r≤2rs}≤K+Cs2.(1)\#\{r\in D(A):r\le2r_s\}\le K+C s^2. \tag{1}

To prove this, fix p∈Ap\in A and cover its radius-2rs2r_s disk by 64 squares of side rs/2r_s/2. Each square has diameter less than rsr_s, so its points determine at most ss distances. If it has at least two points, use two as anchors. Every remaining point is an intersection of one circle about each anchor, with radii chosen among at most ss values. There are at most 2s2+22s^2+2 points in the square. Hence pp has at most 128(s2+1)128(s^2+1) points of AA within distance 2rs2r_s.

Consequently distances at most 2rs2r_s account for at most 64(s2+1)n≤128s2n64(s^2+1)n\le128s^2n unordered pairs. Fewer than 128s2128s^2 of these distance classes can be rich, since each rich class has more than nn pairs. There are at most KK rare classes, proving (1), for example with C=128C=128.

Equilateral zigzags between two convex chains

Suppose p0,…,ptp_0,\ldots,p_t is an xx-monotone path with all edges of length rsr_s. Assume its even vertices follow the lower boundary chain of a strictly convex polygon, its odd vertices follow the upper chain, and successive edges alternate upward and downward. Then

t≤2K+2Cs2+1.(2)t\le 2K+2Cs^2+1. \tag{2}

Let the successive edge directions be θi∈(−π/2,π/2)\theta_i\in(-\pi/2,\pi/2), indexed by 0≤i<t0\le i<t, and set

βi=(−1)i(θi−θi+1)∈(0,π),ϕi=θi+θi+1.\beta_i=(-1)^i(\theta_i-\theta_{i+1})\in(0,\pi), \qquad \phi_i=\theta_i+\theta_{i+1}.

The two-step chord is

pi+2−pi=2rscos⁡(βi/2)eiϕi/2.p_{i+2}-p_i=2r_s\cos(\beta_i/2)e^{i\phi_i/2}.

Strict convexity of the two chains makes ϕ2j\phi_{2j} strictly increasing and ϕ2j+1\phi_{2j+1} strictly decreasing. The identity

ϕi−ϕi+2=(−1)i(βi−2βi+1+βi+2)\phi_i-\phi_{i+2} =(-1)^i(\beta_i-2\beta_{i+1}+\beta_{i+2})

therefore says that (βi)(\beta_i) is strictly concave. Each value occurs at most twice: three equal values would contradict strict concavity at the middle index. The map β↦2rscos⁡(β/2)\beta\mapsto2r_s\cos(\beta/2) is injective on (0,π)(0,\pi), so the t−1t-1 two-step chords determine at least (t−1)/2(t-1)/2 distances. All are at most 2rs2r_s. Apply (1) to obtain (2).

The hypotheses on the zigzag are essential. This does not control all cross-chain edges, numerous small components, or branching in a fixed-rank distance graph. In particular no almost-spanning boundary chain or circle has been deduced from richness. The bound supplies a local restriction for that missing step rather than asserting it.

The author checked the disk count, unordered-pair factor, angle identity, and strict-concavity inference; the argument is author-recorded.

Linear local spectrum for convex sets

If AA is in strictly convex position, the stronger estimate

Qλ:=#{r∈D(A):r≤λrs}≤K+C0λs(λ≥1)(3)Q_\lambda:=\#\{r\in D(A):r\le\lambda r_s\} \le K+C_0\lambda s\qquad(\lambda\ge1) \tag{3}

holds for an absolute constant C0C_0. Here is a perimeter proof. For fixed pp, the subset S=A∩B‾(p,λrs)S=A\cap\overline B(p,\lambda r_s) is in convex position. Its hull perimeter is at most 2πλrs2\pi\lambda r_s, by monotonicity of convex perimeter under inclusion. Partition that boundary into at most ⌈4πλ⌉\lceil4\pi\lambda\rceil arcs of length at most rs/2r_s/2, assigning shared endpoints to just one arc. Each part has diameter at most rsr_s and thus at most ss distinct distances. Altman's convex distance bound gives at most 2s+12s+1 points per part. The cases ∣S∣≤2|S|\le2 are immediate. Therefore pp has O(λs)O(\lambda s) neighbors within distance λrs\lambda r_s. Counting unordered pairs as above proves (3).

Altman's bound is recorded as Theorem 1 in the supplied Fishburn source. For s=1s=1, one can omit it: after normalizing the minimum distance to one, any convex subset in a radius-λ\lambda disk has at most 2πλ2\pi\lambda points, because every hull side has length at least one. This gives Qλ≤K+πλQ_\lambda\le K+\pi\lambda for λ≥1\lambda\ge1, with the sets of at most two points handled directly.

Densely spaced, order-preserving cross matchings

Let p1,…,pmp_1,\ldots,p_m be points of an upper convex chain in left-to-right order and q1,…,qmq_1,\ldots,q_m points of a disjoint lower convex chain in left-to-right order. Assume their directed successive-chord angles lie in one interval of width less than π/2\pi/2, and that

∣pi−qi∣≤rs,∣pi+1−pi∣≤Lrs,|p_i-q_i|\le r_s,\qquad |p_{i+1}-p_i|\le Lr_s,

where L≥1L\ge1. For strictly convex AA with R(A)≤KR(A)\le K,

m≤2QL+2 6+1≤2(K+C0(L+2)s)6+1.(4)m\le2Q_{L+2}^{\,6}+1 \le2\bigl(K+C_0(L+2)s\bigr)^6+1. \tag{4}

All six distances in the ordered quadruple (pi,pi+1,qi,qi+1)(p_i,p_{i+1},q_i,q_{i+1}) are at most (L+2)rs(L+2)r_s, by the triangle inequality. Their ordered list determines the cosine of the relative angle of its two directed chain chords, using

2(b−a)⋅(d−c)=∣a−d∣2+∣b−c∣2−∣a−c∣2−∣b−d∣2.2(b-a)\cdot(d-c) =|a-d|^2+|b-c|^2-|a-c|^2-|b-d|^2.

There are at most QL+26Q_{L+2}^6 lists, and each cosine gives at most two relative angles in the stipulated nonwrapping interval. But the upper chord angles strictly decrease while the lower ones strictly increase, so all m−1m-1 relative angles are distinct. This proves (4). Cross-pair lengths need not be equal.

The author checked the six-distance bound, the polarization identity, and angle monotonicity; the argument is author-recorded. These estimates still do not control numerous isolated or widely separated cross components. Richness has not been converted into the almost-spanning boundary successor structure needed for circular rigidity.

What can be inherited after removing a large convex subset

Let C⊆AC\subseteq A be strictly convex, with m=∣C∣≥cnm=|C|\ge cn, and put I=A∖CI=A\setminus C. The rest of AA need not be convex. Let rsr_s remain the ss-th smallest global distance. For any set BB, let RB(≤t)R_B(\le t) count its occurring distances at most tt whose multiplicities are at most ∣B∣|B|.

The local perimeter proof above works for CC in a disk centered at any point of AA. A disk of radius λrs\lambda r_s contains O(λs)O(\lambda s) points of CC: partition its convex-hull perimeter into O(λ)O(\lambda) arcs of length at most rs/2r_s/2 and use Altman's bound to put at most 2s+12s+1 vertices on each. Thus there are at most C1λsnC_1\lambda s n unordered pairs of length at most λrs\lambda r_s touching CC, for an absolute C1C_1.

A class rare in II but rich in AA must gain at least n+1−∣I∣=m+1n+1-|I|=m+1 such pairs. Therefore

RI(≤λrs)≤RA(≤λrs)+C1λsnm+1≤K+Oc(λs).(5)R_I(\le\lambda r_s) \le R_A(\le\lambda r_s)+\frac{C_1\lambda s n}{m+1} \le K+O_c(\lambda s). \tag{5}

This is a checked local inheritance inequality with the correct threshold ∣I∣|I| on the residual set. It gives no uniform bound for the total R(I)R(I): allowing the cutoff to reach the full diameter can make the error grow with nn. Iterating deletion of large convex layers therefore does not currently yield an induction for the unrestricted problem.

Another attempted step was to turn few short chord lengths on an equilateral convex chain into a periodic sequence of turning angles. No such rigidity lemma was proved. Chord length does not encode the turn word injectively: already the three-step square length 3+2cos⁡α+2cos⁡β+2cos⁡(α+β)3+2\cos\alpha+2\cos\beta+2\cos(\alpha+\beta) is unchanged by reversing the two turns. No adequate bound on the fibers of the longer-word map was established. Moreover, richness has not supplied a long chain with the required boundary order. Neither missing statement should be assumed when using (1)--(5).