2003
DOI: 10.1088/0264-9381/20/11/318
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Poisson structure and symmetry in the Chern–Simons formulation of (2   1)-dimensional gravity

Abstract: In the formulation of (2+1)-dimensional gravity as a Chern-Simons gauge theory, the phase space is the moduli space of flat Poincaré group connections. Using the combinatorial approach developed by Fock and Rosly, we give an explicit description of the phase space and its Poisson structure for the general case of a genus g oriented surface with punctures representing particles and a boundary playing the role of spatial infinity. We give a physical interpretation and explain how the degrees of freedom associate… Show more

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Cited by 71 publications
(170 citation statements)
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References 33 publications
(90 reference statements)
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“…Due to the isomorphism o (2,2) o(2, 1) ⊕ o(2, 1) our results can be also applied to the description of D = 3 AdS symmetries [19]. We recall that o(2, 2) symmetry has been employed in Chern-Simons formulation of D = 3 gravity [20][21][22], with Lorentzian signature and nonvanishing negative cosmological constant. Subsequently, the quantum deformations of D = 3 Chern-Simons theory have been used for the description of D = 3 quantum gravity as deformed D = 3 topological QFT [23,24].…”
Section: Introductionmentioning
confidence: 87%
“…Due to the isomorphism o (2,2) o(2, 1) ⊕ o(2, 1) our results can be also applied to the description of D = 3 AdS symmetries [19]. We recall that o(2, 2) symmetry has been employed in Chern-Simons formulation of D = 3 gravity [20][21][22], with Lorentzian signature and nonvanishing negative cosmological constant. Subsequently, the quantum deformations of D = 3 Chern-Simons theory have been used for the description of D = 3 quantum gravity as deformed D = 3 topological QFT [23,24].…”
Section: Introductionmentioning
confidence: 87%
“…This aspect represents a crucial departure from the four dimensional case and it allows for a different approach to the quantization of the system. In order to clarify this point, let us first recall some basic elements of the inclusion of particles in 3D gravity (see, for instance, [14,[30][31][32][33][34][35] and references therein).…”
Section: Coupling To Massive Point Particlesmentioning
confidence: 99%
“…A description of a moving defect can be obtained by boosting the conical metric, in this case the three momentum of the particle will be a general element of SL(2, R) [3,51]. Various treatments exist for the description of the phase space of point particles coupled to gravity in three dimensions [3,52,53] and its symmetries [54,55].…”
Section: Deforming Momentum Space To the Group Sl(2 R)mentioning
confidence: 99%