Several families of classical integrable systems with two degrees of freedom are derived from phase-space realizations of sl(2) Poisson coalgebras. As a remarkable fact, the existence of the N-dimensional integrable generalization of all these systems is always ensured (by construction) due to their underlying dynamical coalgebra symmetry. By following the same approach, different integrable deformations for such systems are obtained from the q-deformed analogues of sl(2). The well-known Jordan-Schwinger realization is also proven to be related to a (non-coassociative) coalgebra structure on sl(2) and the 2 N dimensional integrable Hamiltonian generated by such Jordan-Schwinger representation is obtained. Finally, the relation between compl...
A classical (or quantum) superintegrable system on an n-dimensional Riemannian manifold is an integr...
We describe of the generalized Drinfeld-Sokolov Hamiltonian reduction for the construction of classi...
We demonstrate the way to derive the second Painlevé equation P2 and its Bäcklund transformations fr...
A universal algorithm to construct N-particle (classical and quantum) completely integrable Hamilton...
A general procedure to get the explicit solution of the equations of motion for N-body classical Ham...
A recently introduced set of N-dimensional quasi-maximally superintegrable Hamiltonian systems descr...
An infinite family of quasi-maximally superintegrable Hamiltonians with a common set of (2N - 3) int...
• Dynamics: cluster variables 3. sl(2)-COALGEBRA SYMMETRY • sl(2)-coalgebra spaces and potentials • ...
A systematic method to construct N-body integrable systems is introduced by means of phase space rea...
A family of classical integrable systems defined on a deformation of the two-dimensional sphere, hyp...
We present a series of results at the interface of cluster algebras and integrable systems, discussi...
We study the geometry of the fibration in invariant tori of a Hamiltonian system which is integrable...
It is shown that the Poisson structure of dynamical systems with three degrees of freedom can be def...
International audienceWe construct a master dynamical system on a U(n) quasi-Poisson manifold, Md, b...
A classical integrable Hamiltonian system is defined by an A belian subalgebra (of suitable dimensio...
A classical (or quantum) superintegrable system on an n-dimensional Riemannian manifold is an integr...
We describe of the generalized Drinfeld-Sokolov Hamiltonian reduction for the construction of classi...
We demonstrate the way to derive the second Painlevé equation P2 and its Bäcklund transformations fr...
A universal algorithm to construct N-particle (classical and quantum) completely integrable Hamilton...
A general procedure to get the explicit solution of the equations of motion for N-body classical Ham...
A recently introduced set of N-dimensional quasi-maximally superintegrable Hamiltonian systems descr...
An infinite family of quasi-maximally superintegrable Hamiltonians with a common set of (2N - 3) int...
• Dynamics: cluster variables 3. sl(2)-COALGEBRA SYMMETRY • sl(2)-coalgebra spaces and potentials • ...
A systematic method to construct N-body integrable systems is introduced by means of phase space rea...
A family of classical integrable systems defined on a deformation of the two-dimensional sphere, hyp...
We present a series of results at the interface of cluster algebras and integrable systems, discussi...
We study the geometry of the fibration in invariant tori of a Hamiltonian system which is integrable...
It is shown that the Poisson structure of dynamical systems with three degrees of freedom can be def...
International audienceWe construct a master dynamical system on a U(n) quasi-Poisson manifold, Md, b...
A classical integrable Hamiltonian system is defined by an A belian subalgebra (of suitable dimensio...
A classical (or quantum) superintegrable system on an n-dimensional Riemannian manifold is an integr...
We describe of the generalized Drinfeld-Sokolov Hamiltonian reduction for the construction of classi...
We demonstrate the way to derive the second Painlevé equation P2 and its Bäcklund transformations fr...