Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Some aspects of geometric quantization and their physical basis

John Andrew Pinto

Published Jan 1, 1987• 0 citations
OpenAlex

Related papers

Geometric Aspects of the Quantization of a Rigid Body

Marco Modugno, Carlos Prieto, Raffaele F. Vitolo

Springer eBooks•Jan 1, 2009•2 citations

Geometric quantization in many-body physics

George Rosensteel

International Journal of Theoretical Physics•Aug 1, 1984•0 citations

A dynamical mechanism for the selection of physical states in ‘geometric quantization schemes’

Paolo Maraner

arXiv:quant-ph/9803063•Reports on Mathematical Physics•Oct 1, 1997•0 citations

Geometric quantization on homogeneous spaces and the meaning of “inequivalent” quantizations

M.A. Robson

arXiv:hep-th/9406057•Physics Letters B•Sep 1, 1994•3 citations

Geometric Quantization and Quantum Mechanics

Jędrzej Śniatycki

Applied mathematical sciences•Jan 1, 1980•463 citations

Bohr-Sommerfeld-Heisenberg Theory in Geometric Quantization

Richard H. Cushman, Jędrzej Śniatycki

In the framework of geometric quantization we extend the Bohr-Sommerfeld rules to a full quantization theory which resembles Heisenberg's matrix theory. This extension is possible because Bohr-Sommerfeld rules not only provide an orthogonal basis in the space of quantum states, but also give a lattice structure to this basis. This permits the definition of appropriate shifting operators. As examples, we discuss the 1-dimensional harmonic oscillator and the coadjoint orbits of the rotation group.

arXiv:1207.1302•Jul 5, 2012•2 citations
In the framework of geometric quantization we extend the Bohr-Sommerfeld rules to a full quantization theory which resembles Heisenberg's matrix theory. This extension is possible because Bohr-Sommerfeld rules not only provide an orthogonal basis in the space of quantum states, but also give a lattice structure to this basis. This permits the definition of appropriate shifting operators. As examples, we discuss the 1-dimensional harmonic oscillator and the coadjoint orbits of the rotation group.