Optical filter and sensor system
An optical filter having a passband at least partially overlapping with a wavelength range of 800 nm to 1100 nm is provided. The optical filter includes a filter stack formed of hydrogenated silicon layers and lower-refractive index layers stacked in alternation. The hydrogenated silicon layers each have a refractive index of greater than 3 over the wavelength range of 800 mn to 1100 nm and an extinction coefficient of less than 0.0005 over the wavelength range of 800 nm to 1100 nm.
1. A method, comprising:
forming a first plurality of layers on a first side of an optical filter,
wherein the first plurality of layers comprises hydrogenated silicon and has a first refractive index of greater than 3 over an operating wavelength range of the optical filter of 800 nanometers (nm) to 1100 nm; and
forming a second plurality of layers on the first side of the optical filter,
wherein the second plurality of layers have a second refractive index of less than 3 over the operating wavelength range of the optical filter of 800 nm to 1100 nm.
2. The method of claim 1 , wherein the first plurality of layers is formed using an inert gas.
3. The method of claim 1 , wherein the second plurality of layers comprises an oxide.
4. The method of claim 1 , wherein between 25 and 48 layers are formed on the first side.
5. The method of claim 1 , wherein the optical filter has a bandpass and the bandpass has a center wavelength that shifts less than 15 nm in magnitude with a change in incidence angle from 0° to 30°.
6. The method of claim 1 , wherein the optical filter is designed for substantially allowing light in a wavelength range that includes the wavelength between 800-1100 nm to pass through the optical filter and exhibits a blocking level greater than OD2 between 400 nm to 1100 nm but outside of the wavelength range.
7. The method of claim 1 , wherein a passband of the optical filter has a full width at half maximum (FWHM) of less than 50 nm.
8. The method of claim 1 , further comprising:
forming a third plurality of layers on the optical filter.
9. The method of claim 8 , wherein the third plurality of layers includes an oxide.
10. The method of claim 8 , wherein the third plurality of layers is formed on a second side of the optical filter.
11. A method, comprising:
sputtering a first silicon target in the presence of hydrogen and an inert gas to deposit a first plurality of layers on a first side of an optical filter,
wherein the first plurality of layers has a first refractive index of greater than 3 over an operating wavelength range of the optical filter of 800 nanometers (nm) to 1100 nm; and
depositing a second plurality of lower-refractive-index layers of the optical filter,
wherein the second plurality of lower-refractive-index layers has a second refractive index of less than 3 over the operating wavelength range of the optical filter of 800 nm to 1100 nm and comprises an oxide.
12. The method of claim 11 , wherein between 25 and 48 layers are formed on the first side.
13. The method of claim 11 , wherein the optical filter has a bandpass and the bandpass has a center wavelength that shifts less than 13 nm in magnitude with a change in incidence angle from 0° to 30°.
14. The method of claim 11 , wherein the optical filter is designed for substantially allowing light in a wavelength range that includes the wavelength between 800-1100 nm to pass through it and exhibits a blocking level greater than OD2 between 400 nm to 1100 nm but outside of the wavelength range.
15. The method of claim 11 , wherein a passband of the optical filter has a full width at half maximum (FWHM) of less than 50 nm.
16. The method of claim 11 , further comprising:
forming a third plurality of layers on the optical filter.
17. The method of claim 16 , wherein the third plurality of layer includes an oxide.
18. The method of claim 16 , wherein the third plurality of layers is formed on a second side of the optical filter.
19. The method of claim 11 , wherein the inert gas is introduced through an anode and a plasma activation source or walls of a vacuum chamber serve as the anode.