AbstractWe consider Chern–Simons theories for the Poincaré, de Sitter and anti-de Sitter groups in three dimensions which generalise the Chern–Simons formulation of 3d gravity. We determine conditions under which κ-Poincaré symmetry and its de Sitter and anti-de Sitter analogues can be associated to these theories as quantised symmetries. Assuming the usual form of those symmetries, with a timelike vector as deformation parameter, we find that such an association is possible only in the de Sitter case, and that the associated Chern–Simons action is not the gravitational one. Although the resulting theory and 3d gravity have the same equations of motion for the gauge field, they are not equivalent, even classically, since they differ in thei...
We construct an action for the superconformal Chern–Simons theory with non-Abelian gauge groups in t...
The equivalence between Chern–Simons and Einstein–Hilbert actions in three dimensions established by...
We show that the Lagrangian for Lovelock–Cartan gravity theory can be reformulated as an action whic...
AbstractWe consider Chern–Simons theories for the Poincaré, de Sitter and anti-de Sitter groups in t...
Abstract We construct a generalisation of the three-dimensional Poincaré algebra that also includes ...
Point particles in 3D gravity are known to behave as topological defects, while gravitational field ...
Point particles in 3D gravity are known to behave as topological defects, while gravitational field ...
These notes summarise a talk surveying the combinatorial or Hamiltonian quantisation of three dimens...
Chamseddine and Mukhanov showed that gravity and gauge theories could be unified in one geometric co...
Abstract Chamseddine and Mukhanov showed that gravity and gauge theories could be unified in one geo...
We construct a generalisation of the three-dimensional Poincar\'e algebra that also includes a colou...
Chern–Simons theories in three dimensions are topological field theories that may have a holographic...
We present a three-dimensional Chern–Simons gravity based on a deformation of the Maxwell algebra. T...
A wide class of three-dimensional gravity models can be put into "Chern-Simons-like" form. We perfor...
A wide class of three-dimensional gravity models can be put into "Chern-Simons-like" form. We perfor...
We construct an action for the superconformal Chern–Simons theory with non-Abelian gauge groups in t...
The equivalence between Chern–Simons and Einstein–Hilbert actions in three dimensions established by...
We show that the Lagrangian for Lovelock–Cartan gravity theory can be reformulated as an action whic...
AbstractWe consider Chern–Simons theories for the Poincaré, de Sitter and anti-de Sitter groups in t...
Abstract We construct a generalisation of the three-dimensional Poincaré algebra that also includes ...
Point particles in 3D gravity are known to behave as topological defects, while gravitational field ...
Point particles in 3D gravity are known to behave as topological defects, while gravitational field ...
These notes summarise a talk surveying the combinatorial or Hamiltonian quantisation of three dimens...
Chamseddine and Mukhanov showed that gravity and gauge theories could be unified in one geometric co...
Abstract Chamseddine and Mukhanov showed that gravity and gauge theories could be unified in one geo...
We construct a generalisation of the three-dimensional Poincar\'e algebra that also includes a colou...
Chern–Simons theories in three dimensions are topological field theories that may have a holographic...
We present a three-dimensional Chern–Simons gravity based on a deformation of the Maxwell algebra. T...
A wide class of three-dimensional gravity models can be put into "Chern-Simons-like" form. We perfor...
A wide class of three-dimensional gravity models can be put into "Chern-Simons-like" form. We perfor...
We construct an action for the superconformal Chern–Simons theory with non-Abelian gauge groups in t...
The equivalence between Chern–Simons and Einstein–Hilbert actions in three dimensions established by...
We show that the Lagrangian for Lovelock–Cartan gravity theory can be reformulated as an action whic...