Abstract:Several issues concerning quantum κ−Poincaré algebra are discussed and reconsidered here. We propose two different formulations of κ−Poincaré quantum algebra. Firstly we present a complete Hopf algebra formulae of κ−Poincaré in classical Poincaré basis. Further by adding one extra generator, which modifies the classical structure of Poincaré algebra, we eliminate non polynomial functions in the κ− parameter. Hilbert space representations of such algebras make Doubly Special Relativity (DSR) similar to the Stue… Show more
“…The above reminds one of some formulas from [39]. This enables us to introduce the new system of generators…”
Section: The Orthogonal D = 1 + ( D − 1) Decomposition Versus the Majmentioning
confidence: 94%
“…In order to preserve a compact form for the formulas (5)- (6) we have also introduced the following notation (extending our previous notation from [39]):…”
Section: Unified Description For κ-Deformationsmentioning
confidence: 99%
“…Drinfeld-Jimbo-type) deformation one can always switch to the so-called q-analog version with all infinite series hidden in the one additional generator. In the case of κ-Poincaré it is −1 τ which solves a specialization problem for κ, for details see [39].…”
Section: Unified Description For κ-Deformationsmentioning
In this paper we provide universal formulas describing Drinfeld-type quantization of inhomogeneous orthogonal groups determined by a metric tensor of an arbitrary signature living in a spacetime of arbitrary dimension. The metric tensor does not need to be in diagonal form and κ-deformed coproducts are presented in terms of classical generators. It opens the possibility for future applications in deformed general relativity. The formulas depend on the choice of an additional vector field which parametrizes classical r -matrices. Non-equivalent deformations are then labeled by the corresponding type of stability subgroups. For the Lorentzian signature it covers three (non-equivalent) Hopf-algebraic deformations: time-like, space-like (a.k.a. tachyonic) and light-like (a.k.a. light-cone) quantizations of the Poincaré algebra. Finally the existence of the so-called Majid-Ruegg (non-classical) basis is reconsidered.
“…The above reminds one of some formulas from [39]. This enables us to introduce the new system of generators…”
Section: The Orthogonal D = 1 + ( D − 1) Decomposition Versus the Majmentioning
confidence: 94%
“…In order to preserve a compact form for the formulas (5)- (6) we have also introduced the following notation (extending our previous notation from [39]):…”
Section: Unified Description For κ-Deformationsmentioning
confidence: 99%
“…Drinfeld-Jimbo-type) deformation one can always switch to the so-called q-analog version with all infinite series hidden in the one additional generator. In the case of κ-Poincaré it is −1 τ which solves a specialization problem for κ, for details see [39].…”
Section: Unified Description For κ-Deformationsmentioning
In this paper we provide universal formulas describing Drinfeld-type quantization of inhomogeneous orthogonal groups determined by a metric tensor of an arbitrary signature living in a spacetime of arbitrary dimension. The metric tensor does not need to be in diagonal form and κ-deformed coproducts are presented in terms of classical generators. It opens the possibility for future applications in deformed general relativity. The formulas depend on the choice of an additional vector field which parametrizes classical r -matrices. Non-equivalent deformations are then labeled by the corresponding type of stability subgroups. For the Lorentzian signature it covers three (non-equivalent) Hopf-algebraic deformations: time-like, space-like (a.k.a. tachyonic) and light-like (a.k.a. light-cone) quantizations of the Poincaré algebra. Finally the existence of the so-called Majid-Ruegg (non-classical) basis is reconsidered.
“…In particular one can choose F µ ( p) in a way leading to classical Poincaré algebra in algebraic sector of κ-deformed Poincaré algebra [33]- [35]. In such a way we get more complicated nonabelian formulae for the composition law of fourmomenta, which unfortunately are not endowed with physical interpretation.…”
The (4 + 4)-dimensional κ-deformed quantum phase space as well as its (10 + 10)-dimensional covariant extension by the Lorentz sector can be described as Heisenberg doubles: the (10 + 10)-dimensional quantum phase space is the double of D = 4 κ-deformed Poincaré Hopf algebra H and the standard (4 + 4)-dimensional space is its subalgebra generated by κ-Minkowski coordinates xµ and corresponding commuting momenta pµ. Every Heisenberg double appears as the total algebra of a Hopf algebroid over a base algebra which is in our case the coordinate sector. We exhibit the details of this structure, namely the corresponding right bialgebroid and the antipode map. We rely on algebraic methods of calculation in Majid-Ruegg bicrossproduct basis. The target map is derived from a formula by J-H. Lu. The coproduct takes values in the bimodule tensor product over a base, what is expressed as the presence of coproduct gauge freedom.
“…Позднее мы на-помним θ-твистованную алгебру Пуанкаре [19], [20]. В завершающей части мы также рассмотрим κ-деформированный дубль Гейзенберга алгебры Пуанкаре [2], но в клас-сическом базисе [21], а не в используемом обычно базисе би-смеш-произведения.…”
Section: модули смеш-произведения и дубли гейзенбергаunclassified
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.