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One off-circle point and concentric polygon constructions


These are restricted results and construction obstructions, not solutions of Problem 132. Pair multiplicities are unordered.

Comparison with two-polygon rich-distance constructions

The independent input, Appendix D.6, correctly warns that constructing many rich classes does not bound the number of rare classes. The established positive-circle theorem says more for Bhowmick's two-polygon constructions: they have linearly many rare classes as well.

In Bhowmick, Section 2, the odd construction has n=2m+1n=2m+1 points and contains a regular (m+1)(m+1)-gon; the even construction has n=2mn=2m points and also contains a regular (m+1)(m+1)-gon. Applying the circle theorem with fraction 1/21/2 gives, respectively,

R(A)≥(n−1)/4−O(n2/3),R(A)≥n/4−O(n2/3).R(A)\ge(n-1)/4-O(n^{2/3}),\qquad R(A)\ge n/4-O(n^{2/3}).

The constants are uniform in the allowed rotation in the odd construction. Thus neither is a bounded-RR family. The source construction and this deduction were checked by the author; the deduction is author-recorded. In counting the selected rich classes, subtract shared unordered pairs, not shared distance values: congruent polygons have the same chord spectrum, but in the reflection case their only shared pair is the common edge. Cross-pairs may further increase multiplicities, so the source's counts are lower bounds for the full classes.

All but one point on a circle

Theorem. If n≥5n\ge5 and n−1n-1 points of AA lie on a circle, then

R(A)≥max⁡{2,⌈n−55⌉}.R(A)\ge\max\left\{2,\left\lceil\frac{n-5}{5}\right\rceil\right\}.

Let H=A∖{p}H=A\setminus\{p\}, h=n−1h=n-1, and normalize its circle to radius one and center zero. A circle distance graph has maximum degree two, so every chord length has at most hh occurrences in HH. Distances from one vertex give at least ⌊h/2⌋\lfloor h/2\rfloor distinct chord lengths. If pp lies on the circle, all distances in AA are rare. Assume first that pp is neither on the circle nor its center. Every distance from pp has at most two occurrences. Richness therefore requires exactly hh occurrences inside HH and exactly two involving pp.

Nonregular circle sets

A chord length with hh occurrences has degree two at every vertex. The corresponding chord rotation preserves HH. If the rotational symmetry group has order gg, then g∣hg\mid h, and the number of potentially rich lengths is at most ⌊(g−1)/2⌋\lfloor(g-1)/2\rfloor; antipodal chords have only h/2h/2 occurrences and cannot be rich. Unless HH is regular, g≤h/2g\le h/2. Thus

R(A)≥⌊h/2⌋−⌊(g−1)/2⌋≥⌊h/4⌋+1.R(A)\ge\lfloor h/2\rfloor-\lfloor(g-1)/2\rfloor \ge\lfloor h/4\rfloor+1.

Regular circle sets: a quantitative argument

If pp is on no reflection axis, all distances from it to HH differ, so no class is rich. Otherwise put p=(ρ,0)p=(\rho,0), ρ>0\rho>0, ρ≠1\rho\ne1, and set m=⌊h/2⌋m=\lfloor h/2\rfloor, δ=2π/h\delta=2\pi/h. The increasing lists of squared chord lengths and distinct squared distances from pp are

S={2−2cos⁡(jδ):1≤j≤m},S=\{2-2\cos(j\delta):1\le j\le m\}, T={1+ρ2−2ρcos⁡((i+α)δ):0≤i<ℓ},T=\{1+\rho^2-2\rho\cos((i+\alpha)\delta):0\le i<\ell\},

where α∈{0,1/2}\alpha\in\{0,1/2\}, ℓ∈{m,m+1}\ell\in\{m,m+1\}, and m+ℓ≥hm+\ell\ge h. The latter assertions follow by folding the regular polygon's angles into [0,π][0,\pi] along its reflection axis.

Put t=∣S∩T∣t=|S\cap T|, a=m−ta=m-t, b=ℓ−tb=\ell-t, and s=a+bs=a+b. Every value in S△TS\triangle T is rare, hence R(A)≥sR(A)\ge s. A match at indices j,ij,i has index difference d=j−(i+1)∈[−b,a]d=j-(i+1)\in[-b,a]: before the match this is the number of unmatched SS entries minus unmatched TT entries. There are at most s+1s+1 such integer differences.

For a fixed dd, put ψ=(d+1−α)δ\psi=(d+1-\alpha)\delta and θ=(i+α)δ\theta=(i+\alpha)\delta. The matching equation is

(cos⁡ψ−ρ)cos⁡θ−sin⁡ψsin⁡θ=(1−ρ2)/2.(\cos\psi-\rho)\cos\theta-\sin\psi\sin\theta =(1-\rho^2)/2.

Its two coefficients cannot both vanish, since ρ>0\rho>0, ρ≠1\rho\ne1. A line intersects the unit circle in at most two points. Thus there are at most two matches for each dd, giving

t≤2(s+1),h≤m+ℓ=2t+s≤5s+4≤5R(A)+4.t\le2(s+1),\qquad h\le m+\ell=2t+s\le5s+4\le5R(A)+4.

Excluding a single rare distance in the regular case

Suppose first h=2m+1h=2m+1 is odd. The star at pp has at least m+1m+1 distinct lengths, but HH has only mm. A unique rare class would therefore be a new star length; every old chord length would have to occur twice in the star. There are 2m+12m+1 star edges, so the new length occurs once. Reflection pairing about the line 0p0p fixes its vertex. Label that vertex (1,0)(1,0) and write p=(ρ,0)p=(\rho,0) with signed ρ\rho. With cj=cos⁡(2πj/h)c_j=\cos(2\pi j/h) this forces

{1+ρ2−2ρcj:1≤j≤m}={2−2cj:1≤j≤m}.\{1+\rho^2-2\rho c_j:1\le j\le m\} =\{2-2c_j:1\le j\le m\}.

The ranges of the two sets give ∣ρ∣=1|\rho|=1, contradicting that pp is off the circle. Here h≥5h\ge5, so the ranges are nonzero.

If h=2mh=2m is even, the polygon diameter is rare: it has at most m+2≤nm+2\le n occurrences after adding pp. Uniqueness of this rare class would force all mm chord lengths to occur twice in the star, with no new length. The reflection axis then has no fixed polygon vertex and passes through opposite edge midpoints. Its folded angles are (2i−1)π/(2m)(2i-1)\pi/(2m), 1≤i≤m1\le i\le m. Put c=cos⁡(π/(2m))c=\cos(\pi/(2m)). Equality of the means of the squared-length sets gives ρ2=1+2/m>1\rho^2=1+2/m>1; equality of their ranges gives 4ρc=4c24\rho c=4c^2, or ρ=c<1\rho=c<1. This contradiction includes h=4h=4.

The center

If p=0p=0, only the circumradius can become rich. Thus R(A)≥⌊h/2⌋−1R(A)\ge\lfloor h/2\rfloor-1, which gives both claimed bounds for h≥6h\ge6. For h=4,5h=4,5, three or more total distances immediately give two rare classes. Suppose there are only two lengths, 1,s1,s. Richness of 11 would require two unit chords in HH.

If the chords share a vertex, their endpoints are three consecutive vertices of a regular hexagon, and s=3s=\sqrt3. A fourth circle point at only distances 1,31,\sqrt3 from those three does not exist: the only remaining candidates relative to the middle vertex are antipodal to one of the other two. If two unit chords are disjoint and no unit chords share a vertex, all four distances between them equal ss. The endpoints of one chord then both lie on the perpendicular bisector of the other; since this line passes through the circle center they are antipodal, contradicting their unit separation. Thus the radius is rare too, completing the proof.

A cocircular hull with two nonvertices

The second independent input, Section 5.3, proves R(A)≥2R(A)\ge2 when exactly two points are nonvertices and the hull vertices are cocircular. The checked unique-diameter theorem shortens its proof and gives the following slightly more general statement.

Proposition. Let AA be an nn-point planar set, n≥5n\ge5, and let C⊂AC\subset A be n−2n-2 points on a circle with center oo. If one point p∈A∖Cp\in A\setminus C lies in conv⁡C\operatorname{conv}C and differs from oo, then R(A)≥2R(A)\ge2. The other point of A∖CA\setminus C is unrestricted.

Write p=∑iαicip=\sum_i\alpha_i c_i as a nontrivial convex combination of points of CC, with positive coefficients. For every c∈Cc\in C,

∣p−c∣2=∑iαi∣ci−c∣2−∑iαi∣ci−p∣2<diam⁡(C)2≤diam⁡(A)2.|p-c|^2 =\sum_i\alpha_i|c_i-c|^2-\sum_i\alpha_i|c_i-p|^2 <\operatorname{diam}(C)^2\le\operatorname{diam}(A)^2.

Since p≠op\ne o, a circle centered at pp meets the circle of CC in at most two points. Thus pp sees at least ⌈(n−2)/2⌉\lceil(n-2)/2\rceil distinct lengths on CC, all strictly below the full diameter, and

q(A)≥⌈(n−2)/2⌉+1.q(A)\ge\lceil(n-2)/2\rceil+1.

If R(A)=1R(A)=1, the pair budget gives q(A)≤⌊n/2⌋q(A)\le\lfloor n/2\rfloor. At odd order these bounds contradict each other. At even order they force q(A)=n/2q(A)=n/2, hence the diameter occurs uniquely, contradicting the unique-diameter theorem. This proves the proposition.

In the stated hull case both remaining points lie in conv⁡C\operatorname{conv}C, and at least one is not the center, so the proposition applies. It includes nonvertex points on hull edges. The independent proof's alternative reflection-pairing argument also checks out, but is not needed once the unique-diameter theorem is available. The author checked both the strict distance exclusion and the parity argument; the argument is author-recorded.

This is a finite-order extension, not a new asymptotic theorem: the positive-circle theorem already gives linear rarity growth for this family. The subsequent all-but-two-circle theorem removes the interior-point assumption altogether: any n−2n-2 concyclic points suffice for R(A)≥2R(A)\ge2. Its proof uses a small-difference lemma and exact regular-polygon palette tests. Arbitrary hulls with two nonvertices remain a separate question, apart from the even-order case covered by that theorem.

Concentric regular rings

The following bounds concern t≥2t\ge2 regular mm-gons with distinct positive circumradii, a common center, and arbitrary rotations. There are n=tmn=tm points. The radii and rotations may depend on mm.

Two rings: a simple uniform bound

Put K=⌊m/2⌋K=\lfloor m/2\rfloor and normalize the radii to 1,r1,r, 0<r<10<r<1. If their within-ring chord spectra have CC common values, each gives

sin⁡(aπ/m)=rsin⁡(bπ/m),1≤a<b≤K.\sin(a\pi/m)=r\sin(b\pi/m),\qquad1\le a<b\le K.

The increasing function f(b)=(m/π)arcsin⁡(rsin⁡(bπ/m))f(b)=(m/\pi)\arcsin(r\sin(b\pi/m)) has f′(b)<1f'(b)<1. Thus the integer gaps b−ab-a strictly increase along these matches. At the jj-th match both a≥ja\ge j and b−a≥jb-a\ge j, so b≥2jb\ge2j. Therefore C≤⌊K/2⌋C\le\lfloor K/2\rfloor.

If the relative rotation is a multiple of π/m\pi/m, there are at most K+1K+1 cross-lengths. The within spectra have 2K−C2K-C values; every one absent from the cross spectrum has at most 2m=n2m=n occurrences. Hence

R(A)≥K−C−1≥⌈K/2⌉−1.R(A)\ge K-C-1\ge\lceil K/2\rceil-1.

Otherwise every cross-length has multiplicity exactly mm, so a rich length must occur in both within spectra. In this case R(A)≥2K−2C≥2⌈K/2⌉R(A)\ge2K-2C\ge2\lceil K/2\rceil. In particular two rings cannot give a bounded-RR sequence as m→∞m\to\infty.

Any fixed number of rings

Put P=t(t+1)/2P=t(t+1)/2 and Cm=12(1+(2m)2/3)C_m=12(1+(2m)^{2/3}). Then

R(A)≥P⌊m/2⌋−P(P−1)Cm.(5)R(A)\ge P\lfloor m/2\rfloor-P(P-1)C_m. \tag{5}

For each unordered radius pair β\beta, its squared-distance spectrum DβD_\beta has at least ⌊m/2⌋\lfloor m/2\rfloor values and the form

Aβ−Bβcos⁡(2πj/m+ηβ),(Aβ,Bβ)=(ri2+rj2,2rirj).A_\beta-B_\beta\cos(2\pi j/m+\eta_\beta),\qquad (A_\beta,B_\beta)=(r_i^2+r_j^2,2r_ir_j).

These parameter pairs are distinct for different unordered radius pairs, since A+B=(ri+rj)2A+B=(r_i+r_j)^2 and A−B=(ri−rj)2A-B=(r_i-r_j)^2. A length belonging to exactly one radius-pair spectrum has multiplicity at most 2m≤n2m\le n, and is rare.

To bound overlaps, fold angles into [0,π][0,\pi], giving at most two translated angular grids for each spectrum. Equality of two values from different spectra gives

y=arccos⁡(a+bcos⁡x),b>0.y=\arccos(a+b\cos x),\qquad b>0.

The sign of the second derivative is the sign of

−abcos⁡2x+(1−a2−b2)cos⁡x−ab.-ab\cos^2x+(1-a^2-b^2)\cos x-ab.

This polynomial vanishes identically only if (a,b)=(0,1)(a,b)=(0,1), which would make the spectra's parameter pairs identical. A singleton overlap domain contributes at most one value. Every nondegenerate domain splits into at most three strictly convex or strictly concave monotone pieces; singular endpoint derivatives do not affect this claim. Scale the coordinates by m/(2π)m/(2\pi). Coincidences lie in a translate of Z2\mathbb Z^2 and have total Manhattan span at most mm.

On one such piece, qq consecutive lattice points have q−1q-1 positive integer gap vectors with distinct slopes, hence distinct vectors. At most (q−1)/2(q-1)/2 positive integer vectors have Manhattan norm at most q−1\sqrt{q-1}. Summing the other vectors' lengths gives m≥(q−1)3/2/2m\ge(q-1)^{3/2}/2, so q≤1+(2m)2/3q\le1+(2m)^{2/3}. Four pairs of angular branches, each split into at most three pieces, give ∣Dβ∩Dγ∣≤Cm|D_\beta\cap D_\gamma|\le C_m.

Finally ∑β∣Dβ∣≥P⌊m/2⌋\sum_\beta|D_\beta|\ge P\lfloor m/2\rfloor. A value in k≥2k\ge2 spectra contributes k≤2(k2)k\le2\binom k2 to this sum. Removing all repeated values leaves at least the right side of (5) values in exactly one spectrum. This proves (5). For fixed tt the bound tends linearly to infinity with mm.

Exact small configurations with R=2R=2

Two concentric squares of radii 11 and q=2−3q=\sqrt{2-\sqrt3}, rotated by π/4\pi/4, have cross squared lengths 1+q2±2q∈{2,2q2}1+q^2\pm\sqrt2q\in\{2,2q^2\}. Each side length has multiplicity 12>812>8, while each of the two diameter lengths has multiplicity two. Thus this eight-point set has R=2R=2, not R≤1R\le1.

Concentric equilateral triangles of radii 1,1/21,1/2, rotated by π/3\pi/3, have multiplicities 9,3,39,3,3 and also R=2R=2. Neither construction refutes an assertion in the question.

The two-square extensions through eleven points

The unrestricted construction attempt tested enlargement of that eight-point example. It cannot produce R=1R=1 by adding at most three points. Here is an exact geometric certificate, independent of a search.

Write a=(3−1)/2a=(\sqrt3-1)/2, c=2−3=2a2c=2-\sqrt3=2a^2, and use the model

B={(±1,0),(0,±1),(±a,±a)}.B=\{(\pm1,0),(0,\pm1),(\pm a,\pm a)\}.

Its inner diameter d=2cd=2\sqrt c has two pairs. Every radius-dd circle contains at most two points of BB. To verify this, all the squared circumradii of its triples belong to

{1,c,2,2/3,2c,2c/3},\{1,c,2,2/3,2c,2c/3\},

none of which equals d2=4cd^2=4c. The outer and inner triples have squared circumradii 1,c1,c. The following mixed triples exhaust the remaining types under the square's symmetry group. Put O1=(1,0),O2=(0,1),O3=(−1,0)O_1=(1,0),O_2=(0,1),O_3=(-1,0) and I+=(a,a),I−=(−a,−a),J=(−a,a),K=(a,−a)I_+=(a,a),I_-=(-a,-a),J=(-a,a),K=(a,-a).

TripleCircumcenterSquared circumradius
O1,O2,I+O_1,O_2,I_+((3+1)/2,(3+1)/2)((\sqrt3+1)/2,(\sqrt3+1)/2)22
O1,O2,I−O_1,O_2,I_-((3−3)/6,(3−3)/6)((3-\sqrt3)/6,(3-\sqrt3)/6)2/32/3
O1,O2,JO_1,O_2,J(a,a)(a,a)2c2c
O1,O3,I+O_1,O_3,I_+(0,−1)(0,-1)22
O1,I+,KO_1,I_+,K(1/3,0)(1/\sqrt3,0)2c/32c/3
O1,J,I−O_1,J,I_-(c,0)(c,0)2c2c
O1,I+,JO_1,I_+,J(0,−1)(0,-1)22
O1,I+,I−O_1,I_+,I_-(a,−a)(a,-a)2c2c

Each center is checked by substituting the three points. For the exhaustion, a pair of outer vertices is adjacent or opposite; the adjacent case has three positions of an inner vertex up to symmetry, and the opposite case has one. The same split for a pair of inner vertices gives the last four rows. All these triples are noncollinear.

If k≤3k\le3 arbitrary points are added, the full multiplicity of dd is at most

2+2k+(k2)≤8+k.2+2k+\binom k2\le8+k.

It remains rare and is not the full diameter, since d<2d<2 and BB already contains a pair of length two. The diameter theorem supplies a second rare class. This excludes only this enlargement strategy, not general sets of eight through eleven points. The author checked the symmetry types, displayed circumcenters, and pair bound; the argument is author-recorded.

The bounds above do not control constructions where both the number of rings and their orders grow without restriction. Nor is there a reduction of arbitrary sets to circular ones.