Summary
The magnetic top (A. O. Barut, M. Bozić and Z. Marić:Ann. Phys. (N.Y.),214, (1992) 53) is quantized using the Bohr-Sommerfeld-Einstein (BSE) and the Einstein-Brillouin-Keller (EBK) quantization methods. It has been previously quantized by canonical, Schrödinger (A. O. Barut, M. Bozić and Z. Marić:Ann. Phys. (N.Y.),214, (1992) 53) and path-integral methods (A. O. Barut and I. Duru:Phys. Lett. A,158, (1991) 441). By comparing the exact wave functions with the semi-classical ones, it is concluded that the usual conditions of quantization should be modified in order to allow for half-integer values of canonical angular momentum (spin). This modification requires to abandon the condition of single-valuedness of wave functions. We justify this using Pauli’s and the Reiss argumentation that single-valuedness of wave functions does not follow from basic quantum-mechanical postulates and that a certain kind of multi-valued (i.e. path-dependent) wave functions cannot be excludeda priori.
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Arsenović, D., Barut, A.O., Marić, Z. et al. Semi-classical quantization of the magnetic top. Nuov Cim B 110, 163–175 (1995). https://doi.org/10.1007/BF02741499
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DOI: https://doi.org/10.1007/BF02741499