2003
DOI: 10.1023/a:1021880025669
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Abstract: We integrate with hyperelliptic functions a two-particle Hamiltonian with quartic potential and additionnal linear and nonpolynomial terms in the Liouville integrable cases 1 : 6 : 1 and 1 : 6 : 8.

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Cited by 7 publications
(2 citation statements)
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“…Note that, in the particular case βγ = 0, i.e. κ 2 1 = κ 2 2 , these coefficients become rational, see [29]. Remark.…”
Section: Equivalent Fourth Order Odesmentioning
confidence: 95%
See 1 more Smart Citation
“…Note that, in the particular case βγ = 0, i.e. κ 2 1 = κ 2 2 , these coefficients become rational, see [29]. Remark.…”
Section: Equivalent Fourth Order Odesmentioning
confidence: 95%
“…In the 1 : 6 : 1, 1 : 6 : 8 case, the hyperelliptic curve y 2 = P (s) of F-VI (see (28)) reduces in the separated cases βγ = 0 to the hyperelliptic curve of the separating variables. Therefore, F-VI is a good ODE to consider, and the only missing item is to find a Hamiltonian structure of F-VI that is necessarily distinct from (30) and admits a canonical transformation to 1 : 6 : 1, 1 : 6 : 8.…”
Section: Conclusion and Unresolved Problemsmentioning
confidence: 99%