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https://doi.org/10.1063/1.531536
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Cite Journal: Journal of Mathematical Physics |  Publication Date: Jun 1, 1996 |
 Citations: 46 |
Affiliation: Université Paris Cité, Sorbonne Université
The dynamical system characterized by the Hamiltonian H(q,p)=âj,k=1n pjpkf(q djâqk) with f(x)=λ+ÎŒ cos(Îœx)+ÎŒâČ sin(Îœâxâ) is completely integrable. Here n is an arbitrary positive integer and λ,ÎŒ,ÎŒâČ,Îœ are 4 arbitrary constants (λ and ÎŒ real, ÎŒâČ and Îœ both real or both imaginary).
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