Nonadiabatic tunneling in an ideal one‐dimensional finite periodic potential system is studied. Resonant transmission, complete reflection which does not exist in the case of ordinary adiabatic tunneling, and acceleration of transmission are analyzed. Some peculiar features resulting from the complete reflection are found and discussed. A system with an impurity is also investigated with an emphasis on the role of complete reflection. The analyses are illustrated by numerical examples.
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© 1992 American Institute of Physics.
1992
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