## Abstract

In classical mechanics, the action and angle variables (J; Θ) can be found by integrating the momentum p with respect to the coordinate q under the constraint of energy conservation. Because it is not known how to extend Riemann integration to operator functions and variables, the classical method of action-angle formalism cannot be extended to quantum mechanics. We show that by using general quantum canonical transformations, one can transform (p; q) into (J; Θ), by which one of the conjugate variables in the Hamiltonian is eliminated. This algebraic integration by quantum canonical transformations gives not only the operator relations between (p; q) and (J; Θ), but also the eigenfunctions of the Hamiltonian and the eigenfunctions of the phase operator. These results offer a new point of view for the action-angle formalism in quantum mechanics.

Original language | English |
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Pages (from-to) | 555-570 |

Number of pages | 16 |

Journal | Chinese Journal of Physics |

Volume | 49 |

Issue number | 2 |

State | Published - Apr 2011 |