Given a manifold , there is a Hilbert space whose elements are square-integrable half-densities on , and whose inner product is given by tensoring two half-densities to an actual density and then integrating that over .
This Hilbert space is often called the canonical Hilbert space of , in contrast with the L-2-spaces of -integrable functions for every choice of measure on .
The notion of canonical Hilbert spaces originates in the context of geometric quantization in (Guillemin-Sternberg). It directly corresponds to the “canonical” construction of groupoid convolution algebras (see there for details) from sections of half-density bundles without choice of a Haar measure.
The notion originates in geometric quantization around
Related lecture notes include
Applications in operator algebra theory appear in
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