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Source. Sections 1.1 (pp. 1-2), 1.2 (p. 2) and 2 (pp. 2-4), with the definitions on pp. 1-3, of Konrad J. Swanepoel, Unit distances and diameters in Euclidean spaces, Discrete Comput. Geom. 41 (2009), no. 1, 1--27, doi:10.1007/s00454-008-9082-x; labels and pages are those of arXiv:0707.0213v1 (2 July 2007), the version named on the source card.

Read depth. Claims checked: each definition was read clause by clause on the printed pages. Nothing here is independently reviewed.

Statement

  • Unit distances (p. 1). For a finite S⊂RdS\subset\mathbb R^d, u(S)u(S) is the number of pairs of points of SS at distance 11, and ud(n)=max⁡{u(S):S⊂Rd, ∣S∣=n}u_d(n)=\max\{u(S):S\subset\mathbb R^d,\ |S|=n\}.
  • Diameters (p. 2). A pair of points of a finite S⊂RdS\subset\mathbb R^d is a diameter when their distance equals the diameter of SS; M(S)M(S) is the number of diameters of SS, and Md(n)=max⁡{M(S):S⊂Rd, ∣S∣=n}M_d(n)=\max\{M(S):S\subset\mathbb R^d,\ |S|=n\}.
  • Lenz configuration, even d≥4d\ge4 (p. 2). Put p=d/2p=d/2 and take any orthogonal decomposition Rd=V1⊕⋯⊕Vp\mathbb R^d=V_1\oplus\cdots\oplus V_p into 22-dimensional subspaces. In each ViV_i let CiC_i be the circle with centre the origin oo and radius rir_i, where ri2+rj2=1r_i^2+r_j^2=1 for all distinct i,ji,j. A Lenz configuration is any translate of a finite subset of ⋃i=1pCi\bigcup_{i=1}^pC_i. For d≥6d\ge6 the radius condition forces every ri=1/2r_i=1/\sqrt2; for d=4d=4 only r12+r22=1r_1^2+r_2^2=1 is required.
  • Lenz configuration, odd d≥5d\ge5 (p. 3). Put p=⌊d/2⌋p=\lfloor d/2\rfloor and take any orthogonal decomposition Rd=V1⊕⋯⊕Vp\mathbb R^d=V_1\oplus\cdots\oplus V_p with V1V_1 of dimension 33 and V2,…,VpV_2,\ldots,V_p of dimension 22. Let Σ\Sigma be the sphere in V1V_1 with centre oo and radius r1r_1, and for i=2,…,pi=2,\ldots,p let CiC_i be the circle in ViV_i with centre oo and radius rir_i, where ri2+rj2=1r_i^2+r_j^2=1 for all distinct i,ji,j. A Lenz configuration is any translate of a finite subset of Σ∪⋃i=2pCi\Sigma\cup\bigcup_{i=2}^pC_i. For d≥7d\ge7 every ri=1/2r_i=1/\sqrt2. The paper notes that this is what its later sections call a strong Lenz configuration, as against the weak Lenz configurations used inside the proofs (Sections 5.3 and 5.4, pp. 11 and 13-14).
  • Extremal set (p. 3). A set SS of nn points of Rd\mathbb R^d is extremal with respect to unit distances when u(S)=ud(n)u(S)=u_d(n), and extremal with respect to diameters when M(S)=Md(n)M(S)=M_d(n).

In a Lenz configuration any two points on different circles (or on the sphere and a circle) are at distance 11; with p=⌊d/2⌋p=\lfloor d/2\rfloor circles of radius 1/21/\sqrt2 and n/p+O(1)n/p+O(1) points on each, this is Lenz's construction of p−12pn2−O(1)\frac{p-1}{2p}n^2-O(1) unit distances recalled on p. 1.

Proof pointer

Definitions; nothing to prove. Section 4 (p. 5) adds the unit distance graph, the counts u(x,S)u(x,S) and u(A,B)u(A,B), and the convention that when diameters are counted the diameter is scaled to 11, so that M(S)=u(S)M(S)=u(S).

Dependencies

None.

Bears on

  • Problem 223: the problem's fd(n)f_d(n), the most pairs at distance one among nn points of diameter one in Rd\mathbb R^d, is the paper's Md(n)M_d(n), since scaling a set to diameter 11 turns its diameters into its pairs at distance 11.
  • Problem 1085: the problem's fd(n)f_d(n) is the paper's ud(n)u_d(n).