Abstract
One of the purposes of geometric quantization (in the sense of Kostant) is to associate in some intrinsic way a finite-dimensional Hilbert space E to a compact symplectic manifold (M, ω) such that \( 2\pi \sqrt {{ - 1}} .\omega \) is the curvature of a connection ∇ on some line bundle L. It is usually assumed that M is simply-connected, since then the pair (L, ∇) is unique up to isomorphism, as was shown in [Ko]. In case there is a finite-dimensional Lie group G of symplectomorphisms present, a central extension \( \mathop{G}\limits^{ \sim } \) of G was constructed by Kostant [Ko], and this central extension should act on E. Thus Kostant was able to recover the Borel-Weil-Bott theorem from the action of a compact Lie group G on a quantizable coadjoint orbit.
Each author was supported in part by a grant from the NSF.
Dedicated to Bert Kostant with admiration
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Brylinski, JL., McLaughlin, D. (1994). Holomorphic Quantization and Unitary Representations of the Teichmüller Group. In: Brylinski, JL., Brylinski, R., Guillemin, V., Kac, V. (eds) Lie Theory and Geometry. Progress in Mathematics, vol 123. Birkhäuser, Boston, MA. https://doi.org/10.1007/978-1-4612-0261-5_2
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