Abstract:Abstract. Families of Perelomov coherent states are defined axiomatically in the context of unitary representations of Hopf algebras. A global geometric picture involving locally trivial noncommutative fibre bundles is involved in the construction. If, in addition, the Hopf algebra has a left Haar integral, then a formula for noncommutative resolution of identity in terms of the family of coherent states holds. Examples come from quantum groups.
“…In his thesis, the present author has developed a direct localization approach ( [15,17]) to the construction of the coset spaces of the quantum linear groups and the locally trivial quantum principal fibrations deforming the classical fibrations of the type G → G/B and having Hopf algebras as the replacements of the structure groups. Apart from the sketch in [15], the main part of that work has been still unpublished (however, a nontrivial application to quantum group coherent states and appropriate measure is exhibited in [16]). The present paper fills a part of this gap in view of the observation that the sets S w in SL q (n) are sets multiplicatively generated by a specific set of quantum minors attached to the permutation matrix w, namely the set of all principal (=lower right corner) quantum minors of the row-permuted matrix of generators T = (t…”
The subset multiplicatively generated by any given set of quantum minors and the unit element in the quantum matrix bialgebra satisfies the left and right Ore conditions.
“…In his thesis, the present author has developed a direct localization approach ( [15,17]) to the construction of the coset spaces of the quantum linear groups and the locally trivial quantum principal fibrations deforming the classical fibrations of the type G → G/B and having Hopf algebras as the replacements of the structure groups. Apart from the sketch in [15], the main part of that work has been still unpublished (however, a nontrivial application to quantum group coherent states and appropriate measure is exhibited in [16]). The present paper fills a part of this gap in view of the observation that the sets S w in SL q (n) are sets multiplicatively generated by a specific set of quantum minors attached to the permutation matrix w, namely the set of all principal (=lower right corner) quantum minors of the row-permuted matrix of generators T = (t…”
The subset multiplicatively generated by any given set of quantum minors and the unit element in the quantum matrix bialgebra satisfies the left and right Ore conditions.
“…The compatibility above ensures that the localization lifts to a localization of (E −Mod) T ([122], 8.5). Hence, T is compatible with the localization in the usual sense, with numerous applications of this type of situation ( [118,120,121,122]). …”
In other to study connections and gauge theories on noncommutative spaces it is useful to use the local trivializations of principal bundles. In this note we show how to use noncommutative localization theory to describe a simple version of cocycle data for the bundles on noncommutative schemes with Hopf algebras in the role of the structure group which locally look like Hopf algebraic smash products. We also show how to use these Čech cocycles for associated vector bundles. We sketch briefly some examples related to quantum groups.
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