Nonlinear optical frequency conversion using metamaterial arrays
US-10054839-B1 · Aug 21, 2018 · US
US11500265B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11500265-B2 |
| Application number | US-201917281814-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 1, 2019 |
| Priority date | Oct 1, 2018 |
| Publication date | Nov 15, 2022 |
| Grant date | Nov 15, 2022 |
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A harmonic light-generating metasurface includes a base substrate and a plurality of structures, that include nonlinear material, that are disposed in a pattern on a surface of the base substrate. Each structure of the plurality of structures individually supports a magnetic dipole mode. An electromagnetic field enhancement of the magnetic dipole mode induces generation of a harmonic signal by the plurality of structures. Alternatively, a harmonic light-generating metasurface, includes a base substrate, a supporting substrate that includes a nonlinear material, and a plurality of paired structures disposed in a pattern on a surface of the supporting substrate. Each paired structure, of the plurality of paired structures, collectively supports a toroidal dipole mode. An electromagnetic field enhancement of the toroidal dipole mode penetrates the supporting substrate to induce generation of a harmonic signal by the supporting substrate.
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What is claimed is: 1. A harmonic light-generating metasurface, comprising: a base substrate; a supporting substrate comprising a nonlinear material; and a plurality of paired structures disposed in a pattern on a surface of the supporting substrate, wherein each paired structure, of the plurality of paired structures, collectively supports a toroidal dipole mode, and an electromagnetic field enhancement of the toroidal dipole mode penetrates the supporting substrate to induce generation of a harmonic signal by the supporting substrate. 2. The harmonic light-generating metasurface of claim 1 , wherein the pattern controls an emission profile of the harmonic signal generated by the plurality of paired structures. 3. The harmonic light-generating metasurface of claim 1 , wherein the pattern is rectilinear. 4. The harmonic light-generating metasurface of claim 1 , wherein the pattern is polar and comprises polar coordinate axes. 5. The harmonic light-generating metasurface of claim 1 , wherein the nonlinear material is a wide-bandgap semiconductor. 6. The harmonic light-generating metasurface of claim 5 , wherein the wide-bandgap semiconductor is indium tin oxide (ITO). 7. The harmonic light-generating metasurface of claim 1 , wherein the plurality of paired structures comprise a plasmonic material. 8. The harmonic light-generating metasurface of claim 1 , wherein the plurality of paired structures are covered by an oxide film disposed on the surface of the supporting substrate. 9. The harmonic light-generating metasurface of claim 1 , wherein the toroidal dipole mode interacts with a second mode of the structure to generate a higher-order multi-pole mode, and the combined toroidal dipole mode electromagnetic fields and high-order multi-pole mode electromagnetic fields penetrate the supporting substrate to induce generation of the harmonic signal. 10. A harmonic light-generating optical system, comprising: a pump laser; and the harmonic light-generating metasurface of claim 1 . 11. The harmonic light-generating optical system according to claim 10 , wherein an ambient atmosphere of the system has access to a first optical path of the pump laser and a second optical path of a harmonic signal generated by the harmonic light-generating metasurface. 12. A method of manufacturing a harmonic light-generating metasurface, the method comprising: disposing a supporting substrate comprising a nonlinear material on a base substrate; and patterning a plurality of paired structures on a surface of the supporting substrate, wherein each paired structure, of the plurality of paired structures, collectively supports a toroidal dipole mode, and an electromagnetic field enhancement of the toroidal dipole mode penetrates the supporting substrate to induce generation of a harmonic signal by the supporting substrate. 13. The method according to claim 12 , wherein patterning the plurality of paired structures comprises: disposing a resist film on the surface of the supporting substrate; pattering the resist film using electron beam lithography; developing the resist film into a mask with a developer; disposing a plasmonic material into and onto the mask; lifting-off the mask with a second developer to leave the pattern of a plurality of paired structures of the plasmonic material directly on the surface of the supporting substrate. 14. The method according to claim 12 , wherein patterning the film comprises stamping the plurality of paired structure onto the surface of the supporting substrate. 15. The method according to claim 12 , wherein the pattern of the plurality of paired structures controls an emission profile of the harmonic signal. 16. The method according to claim 12 , further comprising disposing an oxide film on the surface of the supporting substrate to cover the plurality of paired structures. 17. The method according to claim 12 , wherein the toroidal dipole mode interacts with a second mode of the structure to generate a higher-order multi-pole resonance, and the combined toroidal dipole mode electromagnetic fields and high-order multi-pole electromagnetic fields penetrate the supporting substrate to induce generation of the third harmonic signal by the supporting substrate. 18. The method according to claim 12 , wherein the nonlinear material is a wide-bandgap semiconductor. 19. The method according to claim 18 , wherein the wide-bandgap semiconductor is indium tin oxide (ITO). 20. The method according to claim 12 , wherein the plurality of paired structures comprise a plasmonic material.
Third or higher harmonic generation · CPC title
for second-harmonic generation {(G02F1/3532 takes precedence)} · CPC title
Metamaterials · CPC title
Frequency conversion, i.e. wherein a light beam is generated with frequency components different from those of the incident light beams · CPC title
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