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Solymosi 2008 near optimal bounds erdos distinct distances high dimensions

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corollary_1_2: Theorem 1.1(a) with d0 = 2, d = 3 and Tardos's planar exponent 0.8635 gives g_3(n) = Omega(n^0.5643), improving the bound Omega(n^(77/141 - eps)) of Aronov, Pach, Sharir and Tardos.

corollary_1_3: Theorem 1.1(b) from d0 = 2 for even d and from d0 = 3 for odd d >= 3 gives g_d(n) = Omega(n^(2(d+1)/(d^2+2d-8+6/alpha_2))) and g_d(n) = Omega(n^(2(d+1)/(d^2+2d-15+8/alpha_3))) respectively.

corollary_1_4: For every d >= 4 the least number of distinct distances among n points of R^d is Omega(n^(2/d - 2/(d(d+2)))), against the upper bound O(n^(2/d)) given by the integer lattice.

theorem_1_1: The main theorem of Solymosi and Vu: a power lower bound for the number of distinct distances in dimension d0 yields an explicit power lower bound in every dimension d >= d0, with a second exponent when d - d0 is even.

theorem_2_1: The recursion behind Theorem 1.1(a): if m is the largest number of n given points of R^d, d >= 3, on one hyperplane, some point determines Omega of the larger of n/m^((d-1)/d) and t_{d-1}(m) distinct distances from itself.

theorem_2_2: The recursion behind Theorem 1.1(b): if m is the largest number of n given points of R^d, d >= 3, on one affine subspace of codimension 2, some point determines Omega of the larger of n^((d+1)/2d)/m^((d-1)/2d) and t_{d-2}(m) distinct distances from itself.


J. Solymosi and V. H. Vu, Near optimal bounds for the Erdős distinct distances problem in high dimensions, Combinatorica 28 (2008), no. 1, 113--125; DOI 10.1007/s00493-008-2099-1. The journal data were not checked against the journal.

The copy read for this card is the authors' preprint dated November 11, 2003, 11 pages with a text layer and its own page numbers (181,854 bytes); locators below are its pages. The journal version was not read, and its numbering and statements were not compared with the preprint. The preprint came from a survey download whose URL was not recorded. It prints no copyright or license notice (pp. 1--2 and 10--11 read); no download URL was recorded, so there is no host page to consult, and the journal version was not read; the term is unstated.

Read status: claims checked. Theorem 1.1, Corollaries 1.2--1.4 and Theorems 2.1 and 2.2 were read clause by clause on the page images of pp. 2--3 (the text layer drops plus signs in the exponents); the proofs in sections 2, 4 and 5 were read but not checked step by step.

Contents

Write gd(n)g_d(n) for the minimum number of distinct distances determined by nn points in Rd\mathbb R^d; the lattice gives gd(n)=O(n2/d)g_d(n)=O(n^{2/d}) (p. 1). The introduction (pp. 1--3) recalls, on pp. 1--2, gd(n)=Ω(n1/d)g_d(n)=\Omega(n^{1/d}), the planar bound g2(n)=Ω(n0.8635)g_2(n)=\Omega(n^{0.8635}) of Tardos, g3(n)=Ω(n1/2)g_3(n)=\Omega(n^{1/2}) of Clarkson, Edelsbrunner, Guibas, Sharir and Welzl, and gd(n)=Ω(n1/(d−90/77)−ϵ)g_d(n)=\Omega(n^{1/(d-90/77)-\epsilon}) for d≥3d\ge3 and every ϵ>0\epsilon>0 of Aronov, Pach, Sharir and Tardos.

  • Theorem 1.1 (p. 2; proof in sections 2--5): (a) if gd0(n)=Ω(nαd0)g_{d_0}(n)=\Omega(n^{\alpha_{d_0}}) then for all d≥d0d\ge d_0
gd(n)=Ω(n2d/((d+d0+1)(d−d0)+2d0/αd0));g_d(n)=\Omega\bigl(n^{2d/((d+d_0+1)(d-d_0)+2d_0/\alpha_{d_0})}\bigr);

(b) if gd0(n)=Ω(nαd0)g_{d_0}(n)=\Omega(n^{\alpha_{d_0}}) then for all d≥d0d\ge d_0 with d−d0d-d_0 even

gd(n)=Ω(n2(d+1)/((d+d0+2)(d−d0)+2(d0+1)/αd0)).g_d(n)=\Omega\bigl(n^{2(d+1)/((d+d_0+2)(d-d_0)+2(d_0+1)/\alpha_{d_0})}\bigr).
  • Corollary 1.2 (p. 2): g3(n)=Ω(n0.5643)g_3(n)=\Omega(n^{0.5643}), from (a) with d0=2d_0=2 and Tardos's α2=0.8635\alpha_2=0.8635; the paper announces an improvement to n0.566n^{0.566} by additional arguments.
  • Corollary 1.3 (p. 2): for even dd, gd(n)=Ω(n2(d+1)/(d2+2d−8+6/α2))g_d(n)=\Omega(n^{2(d+1)/(d^2+2d-8+6/\alpha_2)}); for odd d≥3d\ge3, gd(n)=Ω(n2(d+1)/(d2+2d−15+8/α3))g_d(n)=\Omega(n^{2(d+1)/(d^2+2d-15+8/\alpha_3)}).
  • Corollary 1.4 (p. 3): for any d≥4d\ge4, gd(n)=Ω(n2/d−2/(d(d+2)))g_d(n)=\Omega(n^{2/d-2/(d(d+2))}).
  • Section 2 (pp. 3--5) introduces t(A)t(A), the maximum number of distinct distances from one point of AA, states the recursions Theorem 2.1 and Theorem 2.2 (p. 3), which bound t(A)t(A) through the largest number of points of AA on an affine subspace of codimension 1 or 2, and derives Theorem 1.1 from them. Section 3 (pp. 5--6) states a partition lemma of Chazelle and Friedman and its versions (Lemmas 3.2, 3.3 and 3.5), sections 4 (pp. 6--9) and 5 (pp. 9--10) prove Theorems 2.1 and 2.2, and section 6 (p. 10) has concluding remarks, including t(A)=Ω(n2/d−1/d2)t(A)=\Omega(n^{2/d-1/d^2}) for homogeneous sets.

Compiled scope

Only the statements above were checked clause by clause; the derivation in section 2 and the proofs in sections 4 and 5 were read but not checked step by step, and the lemmas of section 3 were not checked. Nothing here is independently reviewed.

Bears on. #1083, as the source of the lower bounds fd(n)≫n2/d−2/(d(d+2))f_d(n)\gg n^{2/d-2/(d(d+2))} for d≥4d\ge4 (Corollary 1.4) and f3(n)≫n0.5643f_3(n)\gg n^{0.5643} (Corollary 1.2), both below the exponent 2/d2/d the problem asks about, so the paper does not answer its question; a sharper d=3d=3 bound quoted on the problem site combines this method with the later Guth--Katz planar bound, which is not in the preprint.

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