2003
DOI: 10.4310/atmp.2003.v7.n6.a3
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The quantisation of Poisson structures arising in Chern-Simons theory with gauge group $G \ltimes \mathfrac{g}^{*}$

Abstract: We quantise a Poisson structure on H n+2g , where H is a semidirect product group of the form G ⋉ g * . This Poisson structure arises in the combinatorial description of the phase space of Chern-Simons theory with gauge group G ⋉ g * on R × S g,n , where S g,n is a surface of genus g with n punctures. The quantisation of this Poisson structure is a key step in the quantisation of Chern-Simons theory with gauge group G ⋉ g * . We construct the quantum algebra and its irreducible representations and show that th… Show more

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Cited by 57 publications
(178 citation statements)
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“…13 This is different from the κ-deformation of the 3+1 Poincaré algebra. 14 This is exactly the Hopf algebra structure of the κ-deformation of the 2+1 Poincaré algebra, or equivalently of the quantum double D(SU (2)), which appears in the quantization of 2+1 gravity [4,17]. The infinitesimal deformation…”
Section: Non-commutative Field Theory As Effective Quantum Gravitymentioning
confidence: 99%
“…13 This is different from the κ-deformation of the 3+1 Poincaré algebra. 14 This is exactly the Hopf algebra structure of the κ-deformation of the 2+1 Poincaré algebra, or equivalently of the quantum double D(SU (2)), which appears in the quantization of 2+1 gravity [4,17]. The infinitesimal deformation…”
Section: Non-commutative Field Theory As Effective Quantum Gravitymentioning
confidence: 99%
“…* is not simply connected, the results of [14,15] can nevertheless be applied to this case 2 and are summarised in the following theorem.…”
Section: Phase Space and Poisson Structurementioning
confidence: 99%
“…3, we briefly review the Hamiltonian version of the Chern-Simons formulation of (2+1)-dimensional gravity. We discuss the role of holonomies and summarise the relevant results of [14,15], in which phase space and Poisson structure are characterised by a symplectic potential on the manifold (P ↑ 3 ) 2g with different copies of P ↑ 3 standing for the holonomies of a set of generators of the fundamental group π 1 (S g ).…”
Section: Introductionmentioning
confidence: 99%
“…Defining a Poincaré element T ∈P ↑ 3 as in (4.10) and setting g = hw −1 , we can rewrite (4.13) as 14) which shows in particular that the kinetic term for the variables associated to the puncture does not depend on the way the coefficient of the curvature singularity (4.9) is parametrised. Moreover, the expression (4.14) has a simple geometric interpretation.…”
Section: The Boundary Condition At Spatial Infinitymentioning
confidence: 99%