Optical modulator with improved efficiency
US-10197821-B2 · Feb 5, 2019 · US
US11683092B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11683092-B2 |
| Application number | US-202117183538-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 24, 2021 |
| Priority date | Feb 24, 2020 |
| Publication date | Jun 20, 2023 |
| Grant date | Jun 20, 2023 |
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A loss-based wavelength meter includes a first photodiode configured to measure power of monochromatic light; and a loss section having a monotonic wavelength dependency, wherein a wavelength of the monochromatic light is determined based on measurements of the first photodiode after the monochromatic light has gone through the loss section. This provides a compact implementation that may be used in integrated optics devices using silicon photonics as well as other embodiments.
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What is claimed is: 1. A loss-based wavelength meter comprising: a first photodiode and a second photodiode each configured to measure power of monochromatic light; and a loss section having a monotonic wavelength dependency, configured to perform evanescent coupling of the monochromatic light for athermality based on the loss section being a waveguide configured with an evanescent coupling mechanism, wherein the loss section is located between the first photodiode and the second photodiode, and wherein a wavelength of the monochromatic light is determined based on a ratio of measurements of the first photodiode and the second photodiode. 2. The loss-based wavelength meter of claim 1 , further comprising a polarizing shaping section. 3. The loss-based wavelength meter of claim 1 , wherein the second photodiode is located before the loss section for an input power measurement. 4. The loss-based wavelength meter of claim 1 , wherein the loss section includes absorbing metal for a wavelength range of interest for the evanescent coupling mechanism. 5. The loss-based wavelength meter of claim 1 , wherein the loss section includes a doped semiconductor for the evanescent coupling mechanism. 6. The loss-based wavelength meter of claim 1 , wherein the loss section includes a semiconductor with a bandgap lower than photon energy in a wavelength range of interest for the evanescent coupling mechanism. 7. The loss-based wavelength meter of claim 1 , wherein the loss section includes Ge for the evanescent coupling mechanism. 8. The loss-based wavelength meter of claim 1 , wherein the loss section includes bend waveguides to assist modal overlap with an adjacent section for the evanescent coupling mechanism. 9. The loss-based wavelength meter of claim 1 , wherein the loss section utilizes coupling into radiative modes through waveguide roughness or waveguide bends. 10. The loss-based wavelength meter of claim 1 , wherein the loss section utilizes light coupling to a substrate. 11. The loss-based wavelength meter of claim 1 , further comprising a plurality of taps for temperature insensitivity based on tap ratios of the plurality of taps. 12. The loss-based wavelength meter of claim 1 , wherein the athermality is over a certain wavelength range. 13. The loss-based wavelength meter of claim 1 , wherein the monochromatic light has an exponential evanescent tail that grows proportionally to the wavelength that extends into a cladding region in the loss section, wherein loss, on the exponential evanescent tail, is exponentially dependent on the wavelength. 14. The loss-based wavelength meter of claim 1 , wherein the loss section has a defined slope for covering a certain wavelength range of interest. 15. The loss-based wavelength meter of claim 14 , wherein the loss section is one of a plurality of loss sections, each of the plurality of loss sections have a defined slope for covering a certain wavelength range of interest. 16. A method of utilizing a loss-based wavelength meter comprising: providing monochromatic light through a loss section having a monotonic wavelength dependency; performing, by the loss section, evanescent coupling of the monochromatic light for athermality based on the loss section being a waveguide configured with an evanescent coupling mechanism, detecting power of the monochromatic light before and after the loss section; and determining a wavelength of monochromatic light based on a ratio of measurements of the power before and after the monochromatic light has gone through the loss section. 17. The method of claim 16 , wherein the determining is based on the measurements after the monochromatic light traverse two different arms of an interferometer. 18. The method of claim 16 , further comprising utilizing a plurality of taps for temperature insensitivity based on tap ratios of the plurality of taps. 19. The method of claim 16 , further comprising combining the measurements with a measurement from a highly accurate but periodic optical reference. 20. The method of claim 16 , wherein the athermality is over a certain wavelength range.
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