2013
DOI: 10.1088/1751-8113/46/28/285203
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From constants of motion to superposition rules for Lie–Hamilton systems

Abstract: A Lie system is a nonautonomous system of first-order differential equations possessing a superposition rule, i.e. a map expressing its general solution in terms of a generic finite family of particular solutions and some constants. Lie-Hamilton systems form a subclass of Lie systems whose dynamics is governed by a curve in a finite-dimensional real Lie algebra of functions on a Poisson manifold. It is shown that Lie-Hamilton systems are naturally endowed with a Poisson coalgebra structure. This allows us to d… Show more

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Cited by 35 publications
(141 citation statements)
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“…This system is important due to the fact that their t -independent constants of motion are employed to obtain a superposition rule for Riccati equations [8]. Let us show first that this system is a Lie system…”
Section: On the Need Of K-symplectic Lie Systemsmentioning
confidence: 99%
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“…This system is important due to the fact that their t -independent constants of motion are employed to obtain a superposition rule for Riccati equations [8]. Let us show first that this system is a Lie system…”
Section: On the Need Of K-symplectic Lie Systemsmentioning
confidence: 99%
“…Nevertheless, Lie systems appear in important physical and mathematical problems and enjoy relevant geometric properties [4,20,23,25,26,30,51,53], which strongly prompt their analysis. Some attention has lately been paid to Lie systems admitting a Vessiot-Guldberg Lie algebra of Hamiltonian vector fields with respect to several geometric structures [7,8,21]. Surprisingly, studying these particular types of Lie systems led to investigate much more Lie systems and applications than before.…”
Section: Introductionmentioning
confidence: 99%
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