2010
DOI: 10.1007/s00220-010-1086-8
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Deformation Quasi-Hopf Algebras of Non-semisimple Type from Cochain Twists

Abstract: One way to obtain Quantized Universal Enveloping Algebras (QUEAs) of non-semisimple Lie algebras is by contracting QUEAs of semisimple Lie algebras. We prove that every contracted QUEA in a certain class is a cochain twist of the corresponding undeformed universal envelope. Consequently, these contracted QUEAs possess a triangular quasi-Hopf algebra structure. As examples, we consider κ-Poincaré in 3 and 4 spacetime dimensions.

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Cited by 7 publications
(14 citation statements)
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“…In this work however we focus mainly on the construction of the Hilbert space of the theory in terms of states labelled by momentum eigenvalues. The reason we focus on this basic aspect is that in analogous four dimensional models a consistent formulation of Fock space has proved to be a surprisingly difficult task [5][6][7][8][9][10]. The results we present here show that in three dimensions a formulation of Fock space consistent with the group nature of momenta and their associated deformed symmetries is in fact possible.…”
Section: Introductionmentioning
confidence: 90%
“…In this work however we focus mainly on the construction of the Hilbert space of the theory in terms of states labelled by momentum eigenvalues. The reason we focus on this basic aspect is that in analogous four dimensional models a consistent formulation of Fock space has proved to be a surprisingly difficult task [5][6][7][8][9][10]. The results we present here show that in three dimensions a formulation of Fock space consistent with the group nature of momenta and their associated deformed symmetries is in fact possible.…”
Section: Introductionmentioning
confidence: 90%
“…-however the cohomological arguments imply the existence of universal Drinfeld twist for D=4 κ-Poincaré [25] we do not have even an explicit formula for Drinfeld twist describing the U q (o(3, 2)) deformation 8 before quantum κ-contraction.…”
Section: Discussion and Outlookmentioning
confidence: 76%
“…We shall show below that it does not exists such f 2 which provides 1 κ 2 terms in the coproducts (25)(26)(27)). Let us notice that due to (28) we get [f 1 , [f 1 , ∆ 0 (N)]] = 0 and we see from (27) that ∆ 2 (N) contains in left factors of tensor product the terms quadratic in P and in right ones the terms linear in N. Such property due to (29) …”
Section: No-go Theorem For D=2mentioning
confidence: 96%
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