Abstract
The Schrodinger equation for an electron near an azimuthally symmetric curved surface in the presence of an arbitrary uniform magnetic field is developed. A thin layer quantization procedure is implemented to bring the electron onto , leading to the well known geometric potential and a second potential that couples , the component of normal to to mean surface curvature, as well as a term dependent on the normal derivative of evaluated on . Numerical results in the form of ground state energies as a function of the applied field in several orientations are presented for a toroidal model.
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