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Central Configuration


For bodies of positive masses m_1,...,m_n at positions q_1,...,q_n, let c be their center of mass and let U(q)=sum_(i<j)m_im_j/||q_i-q_j|| be the Newtonian potential. A collision-free configuration q is a central configuration if there is a number lambda such that

 del _(q_i)U(q)+lambdam_i(q_i-c)=0 for i=1,...,n.

Central configurations generate homographic motions of the bodies. In the plane, each one generates a relative equilibrium that rotates rigidly about the center of mass. They are therefore normally considered up to similarity.

Tomar (2026) proved that, for every choice of four positive masses and every cyclic ordering of the bodies, there is exactly one strictly convex planar central configuration with that ordering, up to similarity. This settles the Simó-Yoccoz conjecture. The proof uses interval arithmetic; the computation was repeated with an independently written program, and the uniqueness theorem and its computation were formalized in Lean and checked by its kernel.

Tomar (2026) states that generative AI tools were used to find and prove the results, write both verification programs and the Lean formalization, and draft the text.


See also

Center of Mass, Similarity, Smale's Problems

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References

Tomar, T. S. "Uniqueness of Four-Body Convex Central Configurations for All Masses." 28 Sep 2026. https://arxiv.org/abs/2609.35632.

Cite this as:

Weisstein, Eric W. "Central Configuration." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/CentralConfiguration.html

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