Saari's homographic conjecture for homogeneous potentials

Let NN point particles have masses mk>0m_k>0 and positions \biqk\bi{q}_k, with homogeneous potential

U=1α1i<jNmimj\biqi\biqjαU=\frac{1}{\alpha}\sum_{1\le i<j\le N}\frac{m_i m_j}{|\bi{q}_i-\bi{q}_j|^\alpha}

for α0\alpha\ne0. Define the moment of inertia and configurational measure by

I=(1i<jNmimj\biqi\biqj2)(k=1Nmk)1,μ=αIα/2U.I=\left(\sum_{1\le i<j\le N}m_i m_j|\bi{q}_i-\bi{q}_j|^2\right)\left(\sum_{k=1}^N m_k\right)^{-1},\qquad \mu=\alpha I^{\alpha/2}U.

Assume that μ\mu is not identically constant. Saari's homographic conjecture. If a motion has constant value of μ\mu, then the motion is homographic. This is the extension of Saari's conjecture to arbitrary homogeneous potentials; the paper proves the claim for general-mass planar three-body motion when α=1\alpha=1 or α=2\alpha=2, while the general statement remains unresolved.

Sources & referencesView supporting material

Primary source

Toshiaki Fujiwara, Hiroshi Fukuda, Hiroshi Ozaki and Tetsuya Taniguchi, “Saari's homographic conjecture for general masses in planar three-body problem under Newton potential and a strong force potential”, arXiv:1503.00407 (2015).

Additional references

2 papers in this index state this conjecture (2009–2015). The statement above is taken from the most recent of them; the others are arXiv:0909.4991.

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