2008
DOI: 10.48550/arxiv.0804.2517
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Construction of quantized enveloping algebras by cocycle deformation

Akira Masuoka

Abstract: By using cocycle deformation, we construct a certain class of Hopf algebras, containing the quantized enveloping algebras and their analogues, from what we call pre-Nichols algebras. Our construction generalizes in some sense the known construction by (generalized) quantum doubles, but unlike in the known situation, it saves us from difficulties in checking complicated defining relations.

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(3 citation statements)
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“…Essential for their result are the Hopf-algebra objects, called Nichols algebras, in the braided tensor category G G YD of Yetter-Drinfel'd modules over a finite abelian group G. In fact, their principle is first to classify the finite-dimensional Nichols algebras L, and then to classify those Hopf algebras which turn, after gr applied, into the bosonizations L >⋖ kG of L by kG. The finite-dimensional pointed Hopf algebras of our concern are those H which are deformed from (L ⊗ R) >⋖ kG by two-cocycle, as in [14] (see also [15]), so that H admits (obviously by construction) the triangular decomposition…”
Section: Introductionmentioning
confidence: 99%
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“…Essential for their result are the Hopf-algebra objects, called Nichols algebras, in the braided tensor category G G YD of Yetter-Drinfel'd modules over a finite abelian group G. In fact, their principle is first to classify the finite-dimensional Nichols algebras L, and then to classify those Hopf algebras which turn, after gr applied, into the bosonizations L >⋖ kG of L by kG. The finite-dimensional pointed Hopf algebras of our concern are those H which are deformed from (L ⊗ R) >⋖ kG by two-cocycle, as in [14] (see also [15]), so that H admits (obviously by construction) the triangular decomposition…”
Section: Introductionmentioning
confidence: 99%
“…which generalizes (1.1). Here, L and R are finite-dimensional Nichols algebras (in positive characteristic, they may be pre-Nichols algebras [14], more generally) which are mutually symmetric in that sense that the braidings between L ⊗ R and R ⊗ L are mutually inverse. The explicit construction of H is given by Proposition 3.3.…”
Section: Introductionmentioning
confidence: 99%
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