Five-body Morse-structure conjecture

Let ff be the function for the equal-mass planar five-body problem, let C5\mathcal{C}_5 be the quotient configuration space, and let P(t)P(t) be its Poincaré polynomial. Five-body Morse-structure conjecture. There are unique values A5(6.755,6.756)A_5\in(6.755,6.756) and Ac(7.5636,7.5638)A_c\in(7.5636,7.5638) such that

M(t)=54+120t+120t2+60t3=P(t)+(1+t)(53+58t+36t2)M(t)=54+120t+120t^2+60t^3=P(t)+(1+t)(53+58t+36t^2)

for 2A<A52\leq A<A_5,

M(t)=150+240t+144t2+60t3=P(t)+(1+t)(149+82t+36t2)M(t)=150+240t+144t^2+60t^3=P(t)+(1+t)(149+82t+36t^2)

for A5<A<AcA_5<A<A_c, and

M(t)=120+240t+174t2+60t3=P(t)+(1+t)(119+112t+36t2)M(t)=120+240t+174t^2+60t^3=P(t)+(1+t)(119+112t+36t^2)

for Ac<AA_c<A. These numerical predictions summarize the proposed bifurcation and Morse-index structure of the five-body problem; their completeness and the asserted transition values remain unproved.

Sources & referencesView supporting material

Primary source

Marshall Hampton, “Planar N-body central configurations with a homogeneous potential”, arXiv:1810.13011 (2019).

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