1983
DOI: 10.1063/1.525703
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Covariance and geometrical invariance in *quantization

Abstract: Several notions of invariance and covariance for * products with respect to Lie algebras and Lie groups are investigated. Some examples, including the Poincaré group, are given. The passage from the Lie-algebra invariance to the Lie-group covariance is performed. The compact and nilpotent cases are treated.

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Cited by 52 publications
(53 citation statements)
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“…x, g (1) (AS(g (2) ) y) = g (2) S(g (3) ) (2) S(g (3) ) * (1) (A * g * (1) x), y = S(g (2) ) * (A * g * (1) x), y , using twice (2.13) and the fact that A is adjointable as well as S ⊗ S • op = • S. This shows that g A is indeed adjointable with adjoint given by (2) ) * A * g (1) …”
Section: Hopf * -Algebras and * -Actionsmentioning
confidence: 99%
“…x, g (1) (AS(g (2) ) y) = g (2) S(g (3) ) (2) S(g (3) ) * (1) (A * g * (1) x), y = S(g (2) ) * (A * g * (1) x), y , using twice (2.13) and the fact that A is adjointable as well as S ⊗ S • op = • S. This shows that g A is indeed adjointable with adjoint given by (2) ) * A * g (1) …”
Section: Hopf * -Algebras and * -Actionsmentioning
confidence: 99%
“…the early work [1]. The resulting general notion of a quantum momentum map is due to [26] but was already used in examples in e.g.…”
Section: Introductionmentioning
confidence: 97%
“…We shall always reserve the symbols u k and v l to denote functions as in (1). Moreover, Karabegov considers locally defined formal series of one-forms α,…”
Section: Karabegov's Description and Characterization Of Star Productmentioning
confidence: 99%
“…that satisfies r(g)J(ξ) = J(Ad(g)ξ) for all g ∈ G and for all ξ ∈ g, clearly defines a quantum momentum mapping which is called a G-equivariant quantum momentum mapping. Also recall the definition of a strongly invariant star product from [1]: Let J 0 be a classical momentum mapping for the action r resp. ̺.…”
Section: Quantum Momentum Mappings For Invariant Star Products Of Wicmentioning
confidence: 99%
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