We search for all Poisson brackets for the BTZ black hole which are consistent with the geometry of the commutative solution and are of lowest order in the embedding coordinates. For arbitrary values for the angular momentum we obtain two two-parameter families of contact structures. We obtain the symplectic leaves, which characterize the irreducible representations of the noncommutative theory. The requirement that they be invariant under the action of the isometry group restricts to R × S1 symplectic leaves, where R is associated with the Schwarzschild time. Quantization may then lead to a discrete spectrum for the time operator
We study certain aspects of noncommutativity in field theory, strings and membranes. We analyse the ...
It has been argued by several authors that the quantum mechanical spectrum of black hole horizon are...
Dynamics with noncommutative coordinates invariant under three dimensional rotations or, if time is ...
We search for all Poisson brackets for the BTZ black hole which are consistent with the geometry of...
We search for all Poisson brackets for the BTZ black hole which are consistent with the geometry of ...
Noncommutative geometry is a candidate for describing physics at the Planck scale. Although there ar...
This note is based on a talk given by one of the authors (S. D.) at the "Rencontres Math\'ematiques ...
Dynamics with noncommutative coordinates invariant under three-dimensional rotations or, if time is ...
We show that a particular noncommutative geometry, sometimes called angular or ρ-Minkowski, requires...
The event horizon of Schwarzschild black hole is obtained in noncommutative spaces up to the second ...
The previous differential calculus on discrete space M. x Z2 which is an underlying space-time in th...
We study the relation between a given set of equations of motion in configuration space and a Poisso...
ABSTRACT: By application of the general twist-induced star-deformation procedure we translate second...
12 pagesWe start from Wootter's construction of discrete phase spaces and Wigner functions for qubit...
We give an interpretation of the Bargmann transform as a correspondence between state spaces that is...
We study certain aspects of noncommutativity in field theory, strings and membranes. We analyse the ...
It has been argued by several authors that the quantum mechanical spectrum of black hole horizon are...
Dynamics with noncommutative coordinates invariant under three dimensional rotations or, if time is ...
We search for all Poisson brackets for the BTZ black hole which are consistent with the geometry of...
We search for all Poisson brackets for the BTZ black hole which are consistent with the geometry of ...
Noncommutative geometry is a candidate for describing physics at the Planck scale. Although there ar...
This note is based on a talk given by one of the authors (S. D.) at the "Rencontres Math\'ematiques ...
Dynamics with noncommutative coordinates invariant under three-dimensional rotations or, if time is ...
We show that a particular noncommutative geometry, sometimes called angular or ρ-Minkowski, requires...
The event horizon of Schwarzschild black hole is obtained in noncommutative spaces up to the second ...
The previous differential calculus on discrete space M. x Z2 which is an underlying space-time in th...
We study the relation between a given set of equations of motion in configuration space and a Poisso...
ABSTRACT: By application of the general twist-induced star-deformation procedure we translate second...
12 pagesWe start from Wootter's construction of discrete phase spaces and Wigner functions for qubit...
We give an interpretation of the Bargmann transform as a correspondence between state spaces that is...
We study certain aspects of noncommutativity in field theory, strings and membranes. We analyse the ...
It has been argued by several authors that the quantum mechanical spectrum of black hole horizon are...
Dynamics with noncommutative coordinates invariant under three dimensional rotations or, if time is ...