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Research notes on every problem, and a library of the papers behind them. Built from the open erdos repository.

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Statement

Setting (p. 165). Pn(k)P_n^{(k)} ranges over the sets of nn distinct points of kk-dimensional Euclidean space with diameter 11; gk(n,r)g_k(n,r) is the largest number of pairs at distance rr among the points of such a set; Gk(n)=max⁡rgk(n,r)G_k(n)=\max_r g_k(n,r) and gk(n)=gk(n,1)g_k(n)=g_k(n,1). So gk(n)g_k(n) is the largest number of times the diameter can occur among nn points of kk-space, and, after rescaling, Gk(n)G_k(n) is the largest number of times any one distance can occur among nn points of kk-space. [x][x] is the integer part.

Theorem (p. 166, unnumbered). For every k≥4k\ge4,

lim⁡n→∞gk(n)n2=lim⁡n→∞Gk(n)n2=12−12[k2].\lim_{n\to\infty}\frac{g_k(n)}{n^2}=\lim_{n\to\infty}\frac{G_k(n)}{n^2} =\frac12-\frac1{2\left[\frac k2\right]}.

The paper reduces the Theorem (p. 166) to two inequalities, using gk(n)≤Gk(n)g_k(n)\le G_k(n) and the monotonicity of gk(n)g_k(n) and Gk(n)G_k(n) in kk: for every l≥2l\ge2,

  • (4) the lower limit of g2l(n)/n2g_{2l}(n)/n^2 is at least 12−12l\frac12-\frac1{2l};
  • (5) the upper limit of G2l+1(n)/n2G_{2l+1}(n)/n^2 is at most 12−12l\frac12-\frac1{2l}.

The print writes plain lim⁡\lim in both (4) and (5); as bounds that are to establish the existence of the limit they are read as the lower and upper limits.

Lenz's construction (3) (pp. 165--166, unpublished result of Lenz, 1955, reported by Erdős). In four-dimensional space, with s=[n/2]s=[n/2], take the ss points (xi,yi,0,0)(x_i,y_i,0,0) and the n−sn-s points (0,0,xj,yj)(0,0,x_j,y_j) with coordinates strictly between 00 and 1/21/\sqrt2 and x2+y2=12x^2+y^2=\frac12 in each case. Every one of the s(n−s)=[n2/4]s(n-s)=[n^2/4] pairs taken from different planes is at distance 11, which is the diameter of the set, so g4(n)≥[n2/4]g_4(n)\ge[n^2/4]. Erdős adds that a slight modification gave Lenz g4(n)>n24+c3ng_4(n)>\frac{n^2}4+c_3n for some c3>0c_3>0, and that Lenz asked for the limit of gk(n)/n2g_k(n)/n^2.

Sharper form (6) (p. 167, stated without proof). From a sharpening of the Erdős--Stone theorem that he says he had recently obtained, Erdős states

Gk(n)<(12−12[k2])n2+O(n2−εk),εk→0 as k→∞.G_k(n)<\left(\frac12-\frac1{2\left[\frac k2\right]}\right)n^2+O(n^{2-\varepsilon_k}), \qquad \varepsilon_k\to0\ \text{as}\ k\to\infty .

He says he does not know how close (6) is to the truth, and suggests that Lenz's lower bound (7), Gk(n)>(12−12[k/2])n2+cknG_k(n)>(\frac12-\frac1{2[k/2]})n^2+c_kn, may give the right order of magnitude. The print sets the denominator of (7) as 2[lk]2[\frac lk] [sic]; the bound (4) and Lenz's construction give [k/2][k/2] there.

Proof pointer

P. 166 for (4), pp. 166--167 for (5).

(4) generalizes Lenz's construction to 2l2l dimensions: for 1≤t≤l1\le t\le l put [n/l][n/l] points on the circle of radius 1/21/\sqrt2 in the plane of coordinates 2t−12t-1 and 2t2t, all with positive coordinates, and zeros elsewhere. Points on different circles are at distance 11, and the whole set has diameter 11, so g2l(n)≥(l2)[n/l]2=n22(1−1l)+O(n)g_{2l}(n)\ge\binom l2[n/l]^2=\frac{n^2}2(1-\frac1l)+O(n).

(5) is by contradiction. If it failed, then for some ε>0\varepsilon>0, some l≥2l\ge2 and infinitely many nn, a set of nn points in 2l+12l+1 dimensions would have more than (12−12l+ε)n2(\frac12-\frac1{2l}+\varepsilon)n^2 pairs at one distance rr. The Erdős--Stone theorem (stated in the footnote on p. 167, reference [6], Bull. Amer. Math. Soc. 52 (1946)) then gives points xi(t)x_i^{(t)}, 1≤i≤31\le i\le3, 1≤t≤l+11\le t\le l+1, with xi1(t1)x_{i_1}^{(t_1)} and xi2(t2)x_{i_2}^{(t_2)} at distance rr whenever t1≠t2t_1\ne t_2. The planes spanned by the triples x1(t),x2(t),x3(t)x_1^{(t)},x_2^{(t)},x_3^{(t)} are then mutually perpendicular, so the points span at least 2l+22l+2 dimensions, which is too many. On p. 167 the print reads "the l+1l+1 planes"; in the scan the subscript of xi2(t2)x_{i_2}^{(t_2)} on the line above hangs beside the ll and can be misread as an exponent, but there is no misprint.

Read depth

Claims checked: the definitions, the Theorem, (3), (4), (5), (6) and (7) were read clause by clause on the page images of the print, and the proofs of (4) and (5) were followed. The perpendicularity step in (5) is called a simple geometrical argument in the print and is not written out there or here. (6) and (7) are stated without proof in the paper. Nothing here is independently reviewed.

Dependencies

None in the corpus. External input named by the paper: the Erdős--Stone theorem (P. Erdős and A. H. Stone, On the structure of linear graphs, Bull. Amer. Math. Soc. 52 (1946), 1087--1091), in the form of the footnote on p. 167.

Source. P. Erdős, On sets of distances of nn points in Euclidean space, Magyar Tud. Akad. Mat. Kutató Int. Közl. 5 (1960), 165--169; the edition read is named on the source card.

Bears on

  • Problem 223: the Theorem's statement for gkg_k gives the problem's fd(n)f_d(n), for every d≥4d\ge4, as (12−12[d/2]+o(1))n2(\frac12-\frac1{2[d/2]}+o(1))n^2; it determines the leading term only, not the exact value. Lenz's (3) is the case d=4d=4 of the lower bound.
  • Problem 1085: the problem's fd(n)f_d(n), the largest number of unit distances among nn points of Rd\mathbb R^d, is Gd(n)G_d(n) after rescaling, so the Theorem gives fd(n)=(12−12[d/2]+o(1))n2f_d(n)=(\frac12-\frac1{2[d/2]}+o(1))n^2 for every d≥4d\ge4. The error terms in (6) and (7) concern the lower-order behaviour; both are stated without proof.