2020/03/24 by Pieter Tibboel, Tibboel, Pieter
Mathematics · Physics and Astronomy · #Algebraic and Geometric Analysis #Classical Analysis and ODEs (math.CA) #FOS: Mathematics #Holomorphic and Operator Theory #Quantum chaos and dynamical systems #Spectral Theory in Mathematical Physics
paper · pdf · doi:10.48550/arxiv.2003.11204
openalex publication_date 2020/03/24 · openalex created_date 2022/07/26 · openalex updated_date 2026/07/28
Let q1,...,qn be the position vectors of the point masses of the\ncurved n-body problem. Consider any positive elliptic-elliptic rotopulsator\nsolution\nqiT=(r\cos(\θ+\αi),r\sin(\θ+\αi),\ρ\cos(\φ+\βi),\ρ\sin(\φ+\βi)),\ni\∈ 1,...,n , where \α1,...,\αn,\β1,...,\βn\∈\n[0,2\π) are constants, \φ, \θ, r and \ρ are\ntwice-differentiable, continuous, nonconstant functions, r2+\ρ2=1,\nr\≥ 0 and \ρ\≥ 0. We prove that the if the configuration of the point\nmasses is of nonconstant size, the configuration of the vectors\n (r\cos(\θ+\αi),r\sin(\θ+\αi))T is a regular\npolygon, as is the configuration of the vectors\n(\ρ\cos(\φ+\βi),\ρ\sin(\φ+\βi))T,\ni\∈ 1,...,n .\n