Abstract

Using the isomorphism {mathfrak {o}}(3;{mathbb {C}})simeq {mathfrak {sl}}(2;{mathbb {C}}) we develop a new simple algebraic technique for complete classification of quantum deformations (the classical r-matrices) for real forms {mathfrak {o}}(3) and {mathfrak {o}}(2,1) of the complex Lie algebra {mathfrak {o}}(3;{mathbb {C}}) in terms of real forms of {mathfrak {sl}}(2;{mathbb {C}}): {mathfrak {su}}(2), {mathfrak {su}}(1,1) and {mathfrak {sl}}(2;{mathbb {R}}). We prove that the D=3 Lorentz symmetry {mathfrak {o}}(2,1)simeq {mathfrak {su}}(1,1)simeq {mathfrak {sl}}(2;{mathbb {R}}) has three different Hopf-algebraic quantum deformations, which are expressed in the simplest way by two standard {mathfrak {su}}(1,1) and {mathfrak {sl}}(2;{mathbb {R}})q-analogs and by simple Jordanian {mathfrak {sl}}(2;{mathbb {R}}) twist deformation. These quantizations are presented in terms of the quantum Cartan–Weyl generators for the quantized algebras {mathfrak {su}}(1,1) and {mathfrak {sl}}(2;{mathbb {R}}) as well as in terms of quantum Cartesian generators for the quantized algebra {mathfrak {o}}(2,1). Finally, some applications of the deformed D=3 Lorentz symmetry are mentioned.

Highlights

  • The search for quantum gravity is linked with studies of noncommutative space-times and quantum deformations of space-time symmetries

  • We recall that in relativistic theories the basic role is played by Lorentz symmetries and the Lorentz algebra, i.e. all aspects of their quantum deformations should be studied in a very detailed and careful way

  • The Lie bialgebra (g, δ) is a correct infinitesimalization of the quantum Hopf deformation of U (g) and the operation δ is an infinitesimal part of the difference between a coproduct and an opposite coproductin the Hopf algebra, δ(x) = h−1( − ̃ ) mod h where h is a deformation parameter

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Summary

Introduction

The search for quantum gravity is linked with studies of noncommutative space-times and quantum deformations of space-time symmetries. 5 all three Hopf-algebraic quantizations (explicit quantum deformations) of the real D = 3 Lorentz symmetry are presented in detail: quantized bases, coproducts and universal R-matrices are given.

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