Abstract
The time-dependent Schrodinger equation describing the resonance interaction of electrons with a radio-frequency (rf) field is solved for asymmetric resonance-tunneling structures with thin, high barriers. It is found that in a number of cases the resonance reflection coefficient of such structures decreases almost to zero as the amplitude of the rf field increases. The conditions under which the largest number of electrons incident on the structure (in a number of cases 100%) interacts efficiently with an rf field with frequency ω and pass into a neighboring resonance level, emitting or absorbing a quantum of energy ħω, are determined.
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