The set of trajectories for massive spinless particles on $AdS_{N+1}$ spacetime is described by the dynamical integrals related to the isometry group SO(2,N). The space of dynamical integrals is mapped one to one to the phase space of the $N$-dimensional oscillator. Quantizing the system canonically, the classical expressions for the symmetry generators are deformed in a consistent way to preserve the $so(2,N)$ commutation relations. This quantization thus yields new explicit realizations of the spin zero positive energy UIR's of SO(2,N) for generic $N$. The representations as usual can be characterized by their minimal energy $\alpha$ and are valid in the whole range of $\alpha$ allowed by unitarity
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
We construct a Lorentz invariant massive particle model in (2+1) space-time with an enlarged set of ...
In this paper we formulate the xp model on the AdS2 spacetime. We find that the spectrum of the Hami...
We analyze AdS3 superparticle dynamics on the coset OSP(1|2)×OSP(1|2)/SL(2,R). The system is quantiz...
Abstract. A complete analysis of the quantum dynamical system defined by the quantum group SL(2,R)&a...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
Abstract We propose a simple unfolded description of free massive higher spin particles in anti-de-S...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
We construct a Lorentz invariant massive particle model in (2+1) space-time with an enlarged set of ...
In this paper we formulate the xp model on the AdS2 spacetime. We find that the spectrum of the Hami...
We analyze AdS3 superparticle dynamics on the coset OSP(1|2)×OSP(1|2)/SL(2,R). The system is quantiz...
Abstract. A complete analysis of the quantum dynamical system defined by the quantum group SL(2,R)&a...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
We compare the respective efficiencies of three quantization methods (group theoretical, coherent st...
Abstract We propose a simple unfolded description of free massive higher spin particles in anti-de-S...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
International audienceWe elaborate the definition and properties of ''massive" elementary systems in...
We construct a Lorentz invariant massive particle model in (2+1) space-time with an enlarged set of ...
In this paper we formulate the xp model on the AdS2 spacetime. We find that the spectrum of the Hami...