ConceptComplete

Geometric Quantization

Geometric quantization is a mathematical framework for constructing quantum Hilbert spaces from classical symplectic manifolds. The moment map plays a central role through the "quantization commutes with reduction" principle.


Prequantization

Definition5.7Prequantum Line Bundle

A prequantization of a symplectic manifold (M,Ο‰)(M, \omega) is a Hermitian line bundle (L,βˆ‡,h)(L, \nabla, h) with connection βˆ‡\nabla whose curvature satisfies curv(βˆ‡)=βˆ’2Ο€iΟ‰\mathrm{curv}(\nabla) = -2\pi i \omega. A prequantization exists if and only if [Ο‰/2Ο€][\omega/2\pi] is an integral cohomology class: [Ο‰]∈H2(M;Z)[\omega] \in H^2(M; \mathbb{Z}).

Definition5.8Polarization

A polarization of (M,Ο‰)(M, \omega) is an integrable Lagrangian distribution PβŠ†TCM\mathcal{P} \subseteq T_\mathbb{C}M (a subbundle of the complexified tangent bundle that is Lagrangian, involutive, and of complex dimension nn). A KΓ€hler polarization is one where P∩Pβ€Ύ=0\mathcal{P} \cap \overline{\mathcal{P}} = 0, corresponding to a compatible complex structure.

ExampleQuantization of $S^2$

For S2S^2 with area form Ο‰=kβ‹…Ο‰std\omega = k \cdot \omega_{\text{std}} (k∈Z>0k \in \mathbb{Z}_{>0}), the prequantum line bundle is O(k)β†’CP1\mathcal{O}(k) \to \mathbb{CP}^1. The quantum Hilbert space (with respect to the KΓ€hler polarization) is H0(CP1,O(k))β‰…Ck+1H^0(\mathbb{CP}^1, \mathcal{O}(k)) \cong \mathbb{C}^{k+1}, a (k+1)(k+1)-dimensional space of degree-kk homogeneous polynomials.


Guillemin-Sternberg Conjecture

RemarkQuantization Commutes with Reduction

The Guillemin-Sternberg conjecture (proved by Meinrenken, Tian-Zhang, and others) states: for a compact Hamiltonian GG-space with prequantum line bundle, the quantization of the reduced space M0=ΞΌβˆ’1(0)/GM_0 = \mu^{-1}(0)/G equals the GG-invariant part of the quantization of MM: Q(M0)β‰…Q(M)G.Q(M_0) \cong Q(M)^G. This is the mathematical formulation of the physical principle that "quantization commutes with reduction."