1993
DOI: 10.1088/0305-4470/26/21/019
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Quantum structure of the motion groups of the two-dimensional Cayley-Klein geometries

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Cited by 72 publications
(97 citation statements)
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“…2 Working within these safe boundaries guarantees that not only the algebra but also the extra structures required for a relativistic theory (such as conservations laws) can be built in a consistent way. We focus on a quantum deformation of the de Sitter algebra (the algebra of isometries of the de Sitter spacetime), known as q-de Sitter [42][43][44][45]. The dimensionless quantum deformation parameter of the q-de Sitter algebra can be fixed as a function of the Planck length l and the de Sitter radius H −1 , and we choose it so that when the Planck length vanishes, the algebra reduces to the de Sitter algebra, while when the de Sitter radius is sent to infinity one recovers the κ-Poincaré Hopf algebra.…”
Section: Introductionmentioning
confidence: 99%
“…2 Working within these safe boundaries guarantees that not only the algebra but also the extra structures required for a relativistic theory (such as conservations laws) can be built in a consistent way. We focus on a quantum deformation of the de Sitter algebra (the algebra of isometries of the de Sitter spacetime), known as q-de Sitter [42][43][44][45]. The dimensionless quantum deformation parameter of the q-de Sitter algebra can be fixed as a function of the Planck length l and the de Sitter radius H −1 , and we choose it so that when the Planck length vanishes, the algebra reduces to the de Sitter algebra, while when the de Sitter radius is sent to infinity one recovers the κ-Poincaré Hopf algebra.…”
Section: Introductionmentioning
confidence: 99%
“…The properties of the nine (1+1)-dimensional geometries corresponding to different signs of κ 1 and κ 2 were investigated in detail in [66] and their (2+1)-dimensional counterparts in [67]. The Lie algebra sl(2, R) is the Cayley-Klein algebra (29) for κ 1 = 1 and κ 2 = −1 with the relation between the bases {P 1 , P 2 , J 12 } and {J ± , J 3 } given by…”
Section: Coisotropic Poisson Homogeneous Spaces For Sl(2 R) ≃ So(2 1)mentioning
confidence: 99%
“…(1) The fundamental LBC's defined by (g (κ 1 ,κ 2 ) , δ (1,1) 02 ) leads to the choice of the transformation law for the deformation parameter (z = √ κ 1 κ 2 w) taken originally for the CK scheme in [18]. In this case, the quantum algebra U w g (κ 1 ,κ 2 ) has coproduct ∆ 02 (3.1) and the following commutation rules…”
Section: Hopf Algebra Contractions Of U Z So(3)mentioning
confidence: 99%