Take the planar three-body problem. Or, said a bit differently,
take that 'cat' to consist of three point masses
moving about in the plane -- a triangle! Fix the center of the mass at the origin
by the usual trick. Take G = SO(2). Now take the quotient and you get the cone over the usual Hopf fibration. The points of the sphere in the base spacerepresent
oriented similarity classes of triangles. This geometry is
at the heart of much modern understanding of the planar three body problem. You can find
references in my 2000 paper with Chenciner
A remarkable periodic solution of the three-body problem in the case of equal masses'
and the geometry explained in some detail in the 1st few pages
and in the appendix to my 1996 paper
The geometric phase of the three-body problem'. You can download these from
http://count.ucsc.edu/~rmont/papers/list.html
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