Metasurface optical components for altering incident light

1. A method of altering incident light using metasurface optical components, the method comprising:

providing a substrate;

depositing metasurface optical components on the surface of the substrate, wherein the metasurface optical components comprise a pattern of silicon dielectric resonators, the silicon dielectric resonators having nonperiodic gap distances between adjacent silicon dielectric resonators, and each silicon dielectric resonator has a width, a length, and a thickness; and

directing incident light to the metasurface optical components, wherein the gap distances, the widths, and the thicknesses are configured to scatter the incident light and impart a phase shift, ranging at least from 0 to 2a, on an outgoing light,

wherein each dielectric resonator has a rectangular cross-section in a plane perpendicular to the substrate surface such that a first phase shift is imparted for a transverse-electric (TE) component of the incident light and a second phase shift is imparted for a transverse-magnetic (TM) component of the incident light.

2. The method of claim 1 , wherein the incident light comprises a wavelength of about 850 nm to 2000 nm.

3. The method of claim 1 , wherein the incident light comprises a wavelength of about 100 nm to 1950 nm.

4. The method of claim 1 , wherein the silicon dielectric resonators comprise amorphous silicon.

5. The method of claim 1 , wherein each of the dielectric resonators have a width of at least 100 nm.

6. The method of claim 1 , wherein the substrate comprises silica.

7. The method of claim 1 , wherein the gap between the dielectric resonators comprises a material with a refractive index lower than the refractive index of the dielectric pillars.

8. The method of claim 1 , wherein the widths of the dielectric resonators and the gaps between adjacent dielectric resonators are configured to deflect a plurality of wavelengths of interest at a shared angle.

9. The method optical device of claim 8 , wherein the first and second phase shifts are different.

10. The method of claim 1 , wherein the nonperiodic gaps are set such that each dielectric resonator is coupled to at least one adjacent dielectric resonator; and the nonperiodic gap size and position define the scattering amplitude and phase.

11. The method of claim 1 , wherein the widths of the dielectric resonators and the gaps between adjacent dielectric resonators are configured to deflect a plurality of wavelengths of interest to or from a focal point at a shared focal length.

12. The method of claim 1 , wherein the widths of the dielectric resonators and the gaps between adjacent dielectric resonators are configured to form a same complex wave-front for a plurality of wavelengths of interest.

13. A metasurface optical device, comprising:

a substrate including a surface; and

a pattern of silicon dielectric resonators on the surface of the substrate,

wherein the silicon dielectric resonators have nonperiodic gap distances between adjacent silicon dielectric resonators, and each silicon dielectric resonator has a width, a length, and a thickness,

wherein the gap distances, the widths, and the thicknesses are configured to scatter incident light and impart a phase shift, ranging at least from 0 to 2π, on an outgoing light, and

wherein each dielectric resonator has a rectangular cross-section in a plane perpendicular to the substrate surface such that a first phase shift is imparted for a transverse-electric (TE) component of the incident light and a second phase shift is imparted for a transverse-magnetic (TM) component of the incident light.

14. The metasurface optical device of claim 13 , wherein the incident light comprises a wavelength of about 850 nm to 2000 nm.

15. The metasurface optical device of claim 13 , wherein the incident light comprises a wavelength of about 1100 nm to 1950 nm.

16. The metasurface optical device of claim 13 , wherein the silicon dielectric resonators comprise amorphous silicon.

17. The metasurface optical device of claim 13 , wherein each of the dielectric resonators have a width of at least 100 nm.

18. The metasurface optical device of claim 13 , wherein the substrate comprises silica.

19. The metasurface optical device of claim 13 , wherein the gap between the dielectric resonators comprises a material with a refractive index lower than the refractive index of the dielectric pillars.

20. The metasurface optical device of claim 13 , wherein the first and second phase shifts are different.

21. The metasurface optical device of claim 13 , wherein the nonperiodic gaps are set such that each dielectric resonator is coupled to at least one adjacent dielectric resonator; and the nonperiodic gap size and position define the scattering amplitude and phase.

22. The metasurface optical device of claim 13 , wherein the widths of the dielectric resonators and the gaps between adjacent dielectric resonators are configured to deflect a plurality of wavelengths of interest to or from a focal point at a shared focal length.

23. The metasurface optical device of claim 13 , wherein the widths of the dielectric resonators and the gaps between adjacent dielectric resonators are configured to deflect a plurality of wavelengths of interest at a shared angle.

24. The metasurface optical device of claim 13 , wherein the widths of the dielectric resonators and the gaps between adjacent dielectric resonators are configured to form a same complex wave-front for a plurality of wavelengths of interest.