Abstract
The explicit quantization of the Lagrangian describing anyon superconductivity is performed using the Dirac-Bergmann method. At first, it is pointed out that it is not possible to choose the gauge-fixing conditiona0 = 0 (with the Coulomb gauge). Secondly, the canonical commutation relations between operators are obtained. Thirdly, the correct effective Hamiltonian is derived. Also, the spontaneous projectivation is discussed. Finally, it is shown that by solving the constraints, the Meissner effect is obtained.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
