Tunable optical group delay based on microresonator structures
View Patent ↗This invention provides a tunable delay of an optical signal having multiple frequency components. The delay comprises at least a first and a second integrated resonators coupled sequentially to a waveguide; the resonators have angular resonant frequencies ω 1 =ω 0 −Δω and ω 2 =ω 0 +Δω respectively, ω 0 is a median frequency of an input optical signal and Δω is a tunable deviation from the median frequency. The device is providing a nearly equal true time delay to all frequency components in the output signal.
1. An optical device for producing a tunable time delay of an input optical signal, comprising:
an optical waveguide receiving the input optical signal;
at least a first loop waveguide resonator coupled to the waveguide by a first coupler, the input signal being coupled in and out of the first loop resonator;
at least a second loop waveguide resonator being coupled to the waveguide by a second coupler; the second loop resonator receiving a signal outputted by the first loop resonator and outputting an output signal;
the output signal being transmitted by the waveguide;
wherein the first and the second loop resonators having different resonant angular frequencies ω 1 and ω 2 , wherein the input optical signal being a complex signal having multiple frequency components, and the device is providing an equal group delay to all frequency components in the output signal.
2. The optical device of claim 1 , wherein the group delay up to 100 ps.
3. The optical device of claim 2 , wherein the group delay up to 1000 ps.
4. The optical device of claim 1 , further comprising the different resonant angular frequencies ω 1 and ω 2 achieved by having different perimeters of the first and second resonators or by different effective refractive indices of the resonator waveguides.
5. The optical device of claim 1 , further comprising:
the resonant angular frequencies ω 1 =ω 0 +Δω and ω 2 =ω 0 −Δω of the loop resonators being equally distant from a frequency ω 0 , wherein ω 0 is an input signal median frequency.
6. The optical device of claim 1 , wherein the resonant angular frequencies ω 1 and ω 2 are tunable.
7. The optical device of claim 6 , wherein the input optical signal being a complex signal having multiple frequency components, and the device is providing an equal tunable group delay to all frequency components in the output signal.
8. The optical device of claim 6 , wherein the resonant angular frequencies .omega.sub.1 and .omega.sub.2 are tunable using thermo-optical effect.
9. The optical device of claim 6 , wherein the resonant angular frequencies ω 1 and ω 2 are tunable using carrier injection.
10. The optical device of claim 6 , wherein the resonant angular frequencies ω 1 and ω 2 are tunable using quantum confined Stark effect.
11. The optical device of claim 6 , wherein the resonant angular frequencies ω 1 and ω 2 are tunable slowly using thermo-optical effect followed by a fast tuning using carrier injection or Stark effect.
12. The optical device of claim 6 , wherein the resonant angular frequencies ω 1 and ω 2 are tunable within a range of +/−0.1% within 10 microsecond.
13. The optical device of claim 6 , wherein coupling rates of first and the second coupler are tunable.
14. The optical device of claim 13 , wherein the coupling rates are tunable using MEMS.
15. The optical device of claim 1 , wherein each of the resonators are ring resonators having a radius ranging from about 2 μm to about 50 μm.
16. The optical device of claim 1 , wherein the first and the second loop resonators are positioned on the opposite sides of the waveguide.
17. The optical device of claim 1 , wherein the device is integrated on silicon or glass or group III-V semiconductor substrate.
18. The optical device of claim 1 , further comprising a first set of resonators having at least twenty resonators and a second set of resonators having at least twenty resonators; each resonator of the first and the second sets of resonators being coupled to the waveguide; the first and the second set of resonators having resonant angular frequencies ω 1 and ω 2 respectively; all resonators being coupled to the waveguide.
19. A method of producing an optical signal delay, the method comprising:
introducing an input optical signal in a waveguide, the optical signal having multiple frequencies;
coupling the optical signal to a first loop resonator;
coupling a light beam outputted by the first resonator to a second loop resonator;
outputting a delayed optical signal, wherein all frequencies of the input optical signal have the same group delay.
20. The method of producing an optical signal delay of claim 19 , wherein:
the first and the second loop resonators having the resonant angular frequencies ω 1 and ω 2 respectively.
21. The method of producing an optical signal delay of claim 19 , further comprising: tuning the resonant angular frequencies ω 1 and ω 2 by the same value resulting in tuning the group delay of the delayed optical signal.
22. The method of producing an optical signal delay of claim 19 , wherein:
the resonant angular frequencies ω 1 =ω 0 +Δω and ω 2 =ω 0 −Δω of the loop resonators being equally distant from the frequency ω 0 , and the input signal having a median frequency ∫ 0 .
23. The method of producing an optical signal delay of claim 19 , further comprising: eliminating a third order group delay dispersion over all frequencies of the input optical signal achieved using cancellation of a positive dispersion of the first loop resonator by a negative dispersion of equal magnitude of the second loop resonator.