Classical and quantum spherical pendulum

dc.contributor.authorCushman, Richard
dc.contributor.authorŚniatycki, Jędrzej
dc.date.accessioned2022-10-27T19:58:21Z
dc.date.available2022-10-27T19:58:21Z
dc.date.copyright2022en_US
dc.date.issued2022
dc.description.abstractThe seminal paper by Niels Bohr followed by a paper by Arnold Sommerfeld led to a revolutionary Bohr–Sommerfeld theory of atomic spectra. We are interested in the information about the structure of quantum mechanics encoded in this theory. In particular, we want to extend Bohr–Sommerfeld theory to a full quantum theory of completely integrable Hamiltonian systems, which is compatible with geometric quantization. In the general case, we use geometric quantization to prove analogues of the Bohr–Sommerfeld quantization conditions for the prequantum operators Pf . If a prequantum operator Pf satisfies the Bohr–Sommerfeld conditions and if it restricts to a directly quantized operator Qf in the representation corresponding to the polarization F, then Qf also satisfies the Bohr–Sommerfeld conditions. The proof that the quantum spherical pendulum is a quantum system of the type we are looking for requires a new treatment of the classical action functions and their properties. For the sake of completeness we have provided an extensive presentation of the classical spherical pendulum. In our approach to Bohr–Sommerfeld theory, which we call Bohr–Sommerfeld–Heisenberg quantization, we define shifting operators that provide transitions between different quantum states. Moreover, we relate these shifting operators to quantization of functions on the phase space of the theory. We use Bohr–Sommerfeld–Heisenberg theory to study the properties of the quantum spherical pendulum, in particular, the boundary conditions for the shifting operators and quantum monodromy.en_US
dc.description.reviewstatusRevieweden_US
dc.description.scholarlevelFacultyen_US
dc.identifier.citationCushman, R. & Śniatycki, J. (2022). “Classical and quantum spherical pendulum.” Symmetry, 14(3), 496. https://doi.org/10.3390/sym14030496en_US
dc.identifier.urihttps://doi.org/10.3390/sym14030496
dc.identifier.urihttp://hdl.handle.net/1828/14349
dc.language.isoenen_US
dc.publisherSymmetryen_US
dc.subjectBohr-Sommerfeld-Heisenberg quantization
dc.subjectgeometric quantization
dc.subjectshifting operators
dc.subject.departmentDepartment of Mathematics and Statistics
dc.titleClassical and quantum spherical pendulumen_US
dc.typeArticleen_US

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