{ "id": "2311.02770", "version": "v1", "published": "2023-11-05T21:00:14.000Z", "updated": "2023-11-05T21:00:14.000Z", "title": "Mass independent shapes for relative equilibria in the two dimensional positive curved three body problem", "authors": [ "Toshiaki Fujiwara", "Ernesto Perez-Chavela" ], "comment": "21 pages, 2 figures", "categories": [ "math.CA" ], "abstract": "In the planar three-body problem under Newtonian potential, it is well known that any masses, located at the vertices of an equilateral triangle generates a relative equilibrium, known as the Lagrange relative equilibrium. In fact, the equilateral triangle is the unique mass independent shape for a relative equilibrium in this problem. The two dimensional positive curved three-body problem, is a natural extension of the Newtonian three-body problem to the sphere $\\mathbb{S}^2$, where the masses are moving under the influence of the cotangent potential. S.~Zhu showed that in this problem, equilateral triangle on a rotating meridian can form a relative equilibria for any masses. This was the first report of mass independent shape on $\\mathbb{S}^2$ which can form a relative equilibrium. % In this paper, we show that, in addition to the equilateral triangle, three isosceles triangles on a rotating meridian, with $\\theta_{ij}=\\theta_{jk}=2^{-1}\\arccos((\\sqrt{2}-1)/2)$ for $(i,j,k)=(1,2,3)$, $(2,3,1)$, $(3,1,2)$ always form relative equilibria for any choice of the masses; where $\\theta_{ij}$ are the angles between the two masses $i$ and $j$ seen from the centre of $\\mathbb{S}^2$. Additionally we prove that, the equilateral and the above three isosceles relative equilibria are unique with this characteristic. We also prove that each relative equilibrium generated by a mass independent shape is not isolated from the other relative equilibria.", "revisions": [ { "version": "v1", "updated": "2023-11-05T21:00:14.000Z" } ], "analyses": { "subjects": [ "70F07", "70F10", "70F15" ], "keywords": [ "relative equilibrium", "equilateral triangle", "unique mass independent shape", "dimensional positive curved three-body problem" ], "note": { "typesetting": "TeX", "pages": 21, "language": "en", "license": "arXiv", "status": "editable" } } }