Abstract

The spectrum of a relativistic electron in a uniform magnetic field is completely analyzed using supersymmetry quantum mechanics. The Dirac Hamiltonian less the rest energy is the supersymmetric Hamiltonian. Not only the electron (or positron) states with opposite helicities, but also the electron and positron states with opposite helicities, are shown to be superpartners. The degeneracy between the electron and positron ground states, as well as excited states with the same helicities, is shown to be due to the spontaneous breaking of symmetry under the combined operation of charge conjugation and time reversal.

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