Journal
APPLIED PHYSICS LETTERS
Volume 118, Issue 18, Pages -Publisher
AMER INST PHYSICS
DOI: 10.1063/5.0048804
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Funding
- Russian Science Foundation [20-19-00559]
- Russian Science Foundation [20-19-00559] Funding Source: Russian Science Foundation
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This study examines the enhancement of surface photoemission from metal into semiconductor through resonance tunneling of photoexcited electrons through (quasi-) discrete levels within the Schottky barrier at the metal-semiconductor interface. The research shows that resonance tunneling can lead to a redshift in the threshold wavelength, higher linear growth in photocurrent near the threshold, and increased efficiency in photoemission, affecting results significantly due to differences in effective masses. Double-barrier tunneling structures with resonant tunneling may be attractive for applications in photochemistry and plasmonic photodetectors in the near IR and middle IR regions of the spectrum.
Enhancement of the surface photoemission from metal into semiconductor by resonance tunneling of photoexcited electrons through (quasi-) discrete level in quantum well, located within Schottky barrier of the metal-semiconductor interface, is studied theoretically taking into account the difference between the electron masses in metal and semiconductor. It is shown, in particular, that resonance tunneling through the discrete level can lead to the redshift of the threshold wavelength of surface photoeffect, higher slope linear growth in photocurrent near the threshold (in contrast to quadratic growth, i.e., Fowler's law), and the possibility to increase substantially the photoemission efficiency similarly to recent experimental results on hot carrier generation in plasmonic structures with a discrete energy level at metal interface. The difference in the effective masses is shown to significantly affect the results. Double-barrier tunneling structures with resonant tunneling may become attractive for applications in photochemistry and in plasmonic photodetectors in near IR and middle IR regions of the spectrum.
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