Abstract

First measurements of time-dependent second-harmonic generation (SHG) at a $\mathrm{S}\mathrm{i}/({\mathrm{ZrO}}_{2}{)}_{x}({\mathrm{SiO}}_{2}{)}_{1\ensuremath{-}x}$ interface show a behavior that is drastically different from similar measurements at ${\mathrm{S}\mathrm{i}/\mathrm{S}\mathrm{i}\mathrm{O}}_{2}$ interfaces. We suggest that in ${\mathrm{S}\mathrm{i}/\mathrm{S}\mathrm{i}\mathrm{O}}_{2}$ only electron injection is important, while both electrons and holes contribute to the dynamics at the $\mathrm{S}\mathrm{i}/({\mathrm{ZrO}}_{2}{)}_{x}({\mathrm{SiO}}_{2}{)}_{1\ensuremath{-}x}$ interface. Multiphoton excitation occurs in Si for all oxides, and involves direct interband transitions. The marked difference between the two systems is related to the population of multiphoton excited states in Si, the corresponding conduction- and valence-band offsets, and trapping/detrapping processes in the oxides. Our measurements confirm the existence of an initial built-in field at the interface.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.