2018
DOI: 10.1090/proc/14263
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On the Fejes Tóth problem about the sum of angles between lines

Abstract: In 1959 Fejes Tóth posed a conjecture that the sum of pairwise non-obtuse angles between N unit vectors in S d is maximized by periodically repeated elements of the standard orthonormal basis. We obtain new improved upper bounds for this sum, as well as for the corresponding energy integral. We also provide several new approaches to the only settled case of the conjecture: d = 1.arXiv:1801.07837v1 [math.MG]

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Cited by 15 publications
(13 citation statements)
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References 12 publications
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“…where to obtain (11) we used (9), and where u on the last line is any fixed point in X . Substituting (9) and (11) into (8) and rearranging, we obtain (7).…”
mentioning
confidence: 99%
“…where to obtain (11) we used (9), and where u on the last line is any fixed point in X . Substituting (9) and (11) into (8) and rearranging, we obtain (7).…”
mentioning
confidence: 99%
“…Not only is Proposition 1.1 limited to even p's, but it is also not trivial to find spherical t-designs for large t. More generally, and to the best of our knowledge, little is known about the complete solutions to (4) even in the simplest case d = 2. When N = 3, a solution is given in [13] for all positive p. See also [6,19] for related results. For any N and p = ∞, it is shown in [5] that the Grassmannian frame is (10) X…”
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confidence: 99%
“…He proved this conjecture for at most 6 lines, and he also gave an upper bound for the sum of angles for an arbitrary number of lines. Our main result of Chapter 2 is Theorem 2.1 in which we give an upper bound for the sum of the angles of n lines in 3-dimensional space, thus improving the general bound of L. Fejes Tóth for large n. We note that after our paper had been published, Bilyk and Matzke [BM19] further improved the upper bound using a different method.…”
Section: Chapter 1 Forewordmentioning
confidence: 79%
“…This means that the sum of angles is asymptotically less than n 2 π/5 as n → ∞. In our paper [FVZ16b], we improved this upper bound to 3n 2 π/16 ≈ 0.589 • n 2 , and later Bilyk and Matzke [BM19] further improved it to π 4 − 69 100d n 2 as n → ∞. We note that their result for d = 3 gives asymptotically less than 0.556 • n 2 as n → ∞.…”
Section: Proof Of Theorem 57mentioning
confidence: 85%
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