Abstract
By using the spherical coordinates in (3+1) dimensions we study the self-adjointness of the Dirac–Hamiltonian in an Aharonov–Bohm gauge field of an infinitely thin magnetic fluxtube. It is shown that the angular part of the Dirac–Hamiltonian requires self-adjoint extensions. These self-adjoint extensions are parametrized by a 2×2 unitary matrix.
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