Abstract

Quantum homogeneous spaces are noncommutative spaces with quantum group covariance. Their semiclassical counterparts are Poisson homogeneous spaces, which are quotient manifolds of Lie groups M = G/H equipped with an additional Poisson structure π which is compatible with a Poisson–Lie structure Π on G. Since the infinitesimal version of Π defines a unique Lie bialgebra structure δ on the Lie algebra , we exploit the idea of Lie bialgebra duality in order to study the notion of complementary dual homogeneous space M ⊥ = G*/H ⊥ of a given homogeneous space M with respect to a coisotropic Lie bialgebra. Then, by considering the natural notions of reductive and symmetric homogeneous spaces, we extend these concepts to M ⊥ thus showing that an even richer duality framework between M and M ⊥ arises from them. In order to analyze physical implications of these notions, the case of M being a Minkowski or (anti-) de Sitter Poisson homogeneous spacetime is fully studied, and the corresponding complementary dual reductive and symmetric spaces M ⊥ are explicitly constructed in the case of the well-known κ-deformation, where the cosmological constant Λ is introduced as an explicit parameter in order to describe all Lorentzian spaces simultaneously. In particular, the fact that M ⊥ is a reductive space is shown to provide a natural condition for the representation theory of the quantum analogue of M that ensures the existence of physically meaningful uncertainty relations between the noncommutative spacetime coordinates. Finally, despite these dual spaces M ⊥ are not endowed in general with a G*-invariant metric, we show that their geometry can be described by making use of K-structures.

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