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Centres of mass, Steiner's theorem, and equations of Erdős-Moser type

Elham Mehdi-Nezhad, Amir M. Rahimi

Source record

Source: arXiv

Published: Oct 29, 2026

arXiv: 2610.39315

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Source abstract

We study the Erdős--Moser equation 1k+2k+⋯+(m−1)k=mk1^k+2^k+\dots+(m-1)^k=m^k and its analogue in arithmetic progressions, ∑i<m, i≡b(modq)ik=mk\sum_{i<m,\ i\equiv b \pmod q} i^k=m^k, by means of centres of mass, through what we call the half-mass principle. For the progression equation we show that a solution with exponent kk has at most ⌊k/log⁡2+3/2⌋\lfloor k/\log 2+3/2\rfloor terms for all k<1055k<10^{55}, which is best possible for real solutions and replaces an exponential bound; that for k=3k=3 solutions with exactly nn terms exist if and only if n∈{3,4,5}n\in\{3,4,5\}, and then infinitely many; and that there are no solutions at all for k=4k=4, more generally for every k=2s≥4k=2^s\ge 4, and for every even kk with 4≤k≤244\le k\le 24. These results rest on a uniform estimate for the Erdős--Moser equation: the real exponent κmκ_m for which 1κ+⋯+(m−1)κ=mκ1^κ+\dots+(m-1)^κ=m^κ satisfies κm=log⁡2 (m−3/2−γm/m)κ_m=\log 2\,(m-3/2-γ_m/m) with 0<γm<1/(8log⁡2)0<γ_m<1/(8\log 2) for every m≥3m\ge 3. The method also explains the constants: 3/23/2 is a Steiner quotient (ρ2+d2)/2d(ρ^2+d^2)/2d, and 25/12−3log⁡2=1/12−f′′(log⁡2)/225/12-3\log 2=1/12-f''(\log 2)/2 with f(λ)=λ/(eλ−1)f(λ)=λ/(e^λ-1), which explains why this number is so small.

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