Superintegrable systems on 3-dimensional curved spaces: Eisenhart formalism and separability

In this paper (arXiv:1701.05783) the Eisenhart geometric formalism, which transforms an Euclidean natural Hamiltonian into a geodesic Hamiltonian with one additional degree of freedom, is applied to the four families of quadratically superintegrable systems with multiple separability in the Euclidean plane. Firstly, the separability and superintegrability of such four geodesic Hamiltonians in a three-dimensional curved space are studied and then these four systems are modified with the addition of a potential. Secondly, we study the superintegrability of certain four position-dependent mass Hamiltonians, that enjoys the same separability as the original system. All the Hamiltonians here studied describe superintegrable systems on non-Euclidean three-dimensional manifolds with a broken spherically symmetry.


AdS Poisson homogeneous spaces and Drinfel’d doubles

In this paper (arXiv:1701.04902) the correspondence between Poisson homogeneous spaces over a Poisson-Lie group G and Lagrangian Lie subalgebras of the classical double D(𝔤) is revisited and explored in detail for the case in which 𝔤=D(𝔞) is a classical double itself. We apply these results to give an explicit description of all 2d Poisson homogeneous spaces over the group SL(2,R)≅SO(2,1), namely 2d anti de Sitter space, 2d hyperbolic space and the lightcone in 3d Minkowski space. We show how each of these spaces is obtained as a quotient with respect to a Poisson-subgroup for one of the three inequivalent Lie bialgebra structures on sl(2,R) and as a coisotropic one for the others. We then classify the Poisson homogeneous structures for 3d anti de Sitter space AdS3 and show that the ones that are quotients by a Poisson subgroup are determined by a three-parameter family of classical r-matrices for so(2,2), while the coisotropic cases are much more numerous. In particular, we present the two Poisson homogeneous structures on AdS3 that arise from two Drinfel’d double structures on SO(2,2). The first one realises AdS3 as a quotient of SO(2,2) by the Poisson-subgroup SL(2,R), while the second one, the non-commutative spacetime of the twisted κ-AdS deformation, realises AdS3 as a coisotropic Poisson homogeneous space.

Lie Hamilton systems on curved spaces: A geometrical approach

A Lie-Hamilton system is a nonautonomous system of first-order ordinary differential equations describing the integral curves of a t-dependent vector field taking values in a finite-dimensional Lie algebra, a Vessiot-Guldberg Lie algebra, of Hamiltonian vector fields relative to a Poisson structure. Their general solution can be written as an autonomous function, the superposition rule, of a generic finite family of particular solutions and a set of constants. In this paper (arXiv:1612.08901) we pioneer the study of Lie-Hamilton systems on Riemannian spaces (sphere, Euclidean, and hyperbolic plane), pseudo-Riemannian spaces (anti-de Sitter, de Sitter, and Minkowski spacetimes) as well as on semi-Riemannian spaces (Newtonian spacetimes). Their corresponding constants of motion and superposition rules are obtained explicitly in a geometric way. This work extends the (graded) contraction of Lie algebras to a contraction procedure for Lie algebras of vector fields, Hamiltonian functions, and related symplectic structures, invariants, and superposition rules.

The kappa-(A)dS quantum algebra in (3+1) dimensions

In this paper (arXiv:1612.03169) the quantum duality principle is used to obtain explicitly the Poisson analogue of the kappa-(A)dS quantum algebra in (3+1) dimensions as the corresponding Poisson-Lie structure on the dual solvable Lie group. The construction is fully performed in a kinematical basis and deformed Casimir functions are also explicitly obtained. The cosmological constant Λ is included as a Poisson-Lie group contraction parameter, and the limit Λ0 leads to the well-known kappa-Poincaré algebra in the bicrossproduct basis. A twisted version with Drinfel’d double structure of this kappa-(A)dS deformation is sketched.

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