Tunable resonator-based devices for producing variable delays and narrow spectral linewidths

• US 7,024,069 B2
• Filed: 10/01/2004
• Issued: 04/04/2006
• Est. Priority Date: 10/01/2003
• Status: Active Grant

• Current Assignee: California Institute of Technology
• Original Assignee: California Institute of Technology
• Inventors: Matsko, Andrey B., Ilchenko, Vladimir, Savchenkov, Anatoliy, Maleki, Lutfollah
• Primary Examiner(s): Kianni, Kaveh
• Assistant Examiner(s): Kalivoda, Christopher M.
• Application Number:
  US10/956,876
• Publication Number:
  US 20050074200A1
• Time in Patent Office: 550 Days
• Field of Search: 385/1, 385/14, 385/15, 385/16, 385/24, 385/28, 385/30, 385/50, 385129-132
• US Class Current: 385/15
• CPC Class Codes: G02B 2006/12109 Filter
• CPC Class Codes: G02B 6/12007 forming wavelength selective elements, e.g. multiplexer, demultiplexer

Abstract

Devices with two or more coupled resonators to produce narrow spectral responses due to interference of signals that transmit through the resonators and techniques for operating such devices to achieve certain operating characteristics are described. The devices may be optical devices where optical resonators such as whispering gallery mode resonators may be used. In one implementation, at least one of the coupled optical resonators is a tunable resonator and is tuned to change its resonance frequency to tune the spectral response of the device. The described devices and techniques may be applied in optical filters, optical delays, optical waveform generators, and other applications.

Claims

1. A method, comprising:

optically coupling a first optical resonator with a first resonance frequency to first and second optical waveguides, wherein the first optical resonator is tunable to change the first resonance frequency;

optically coupling a second optical resonator with a second resonance frequency to the first and second optical waveguides to cause an optical interference between optical signals that transmit through the first and second optical resonators via the first and second waveguides to produce a narrow spectral transmission peak centered at an average frequency of the first and the second resonance frequencies; and

tuning the first optical resonator to change a difference between the first and second resonance frequencies to change an optical delay of light in the transmission peak.

2. The method as in claim 1, further comprising tuning the first optical resonator to change a sum of the first and second resonance frequencies and to tune the transmission peak in frequency.

3. The method as in claim 1, further comprising using a first whispering gallery mode resonator as the first optical resonator and a second whispering gallery mode resonator as the second optical resonator.

4. The method as in claim 1, wherein the second optical resonator is tunable to change the second resonance frequency, and the method further comprising tuning the second optical resonator, in addition to tuning the first optical resonator, to change the difference between the first and second resonance frequencies.

5. The method as in claim 4, further comprising tuning at least one of the first and second optical resonators to change a sum of the first and second resonance frequencies and to tune the transmission peak in frequency.

6. The method as in claim 4, wherein each of the first and second optical resonators is a tunable electro-optic optical resonator.

7. The method as in claim 1, wherein the first optical resonator is a tunable electro-optic optical resonator.

8. The method as in claim 1, further comprising placing the first and second optical resonators relative to each other so that the first and second optical resonators are not directly optically coupled to each other and are optically coupled via optical coupling to the first and second waveguides.

9. The method as in claim 1, further comprising placing the first and second optical resonators relative to each other so that the first and second optical resonators are directly optically coupled to each other in addition to optical coupling with each other via optical coupling to the first and second waveguides.

10. The method as in claim 9, further comprising controlling the direct coupling between the first and second optical resonators to make the transmission peak a third-order filter function.

11. The method as in claim 1, further comprising optically coupling at least a third optical resonator with a third resonance frequency to the first and second optical waveguides to cause an optical interference with optical signals that transmit through the first, second, and third optical resonators via the first and second waveguides.

12. The method as in claim 1, further comprising tuning the first optical resonator to change a linewidth of the transmission peak from hundreds of kilohertz to several GigaHertz.

13. The method as in claim 1, further comprising controlling optical coupling of the first and second optical resonators, and the first and second waveguides to make a linewidth of the transmission peak to be less than a linewidth of each of the first and second optical resonators.

14. A device, comprising:

a first optical resonator with a first resonance frequency that is tunable to change the first resonance frequency;

a first optical waveguide optically coupled to the first optical resonator;

a second optical waveguide optically coupled to the first optical resonator;

a second optical resonator with a second resonance frequency and optically coupled to the first and second optical waveguides, respectively, to cause an optical interference between optical signals that transmit through the first and second optical resonators via the first and second waveguides to produce a narrow spectral transmission peak centered at an average frequency of the first and the second resonance frequencies; and

a tuning mechanism to tune the first optical resonator to change a difference between the first and second resonance frequencies to change an optical delay of light in the transmission peak.

15. The device as in claim 14, wherein the first and second optical resonators are whispering gallery mode resonators.

16. The device as in claim 14, wherein the second optical resonator is tunable to change the second resonance frequency.

17. The device as in claim 16, wherein the tuning mechanism operates to tune at least one of the first and second optical resonators to change a sum of the first and second resonance frequencies and to tune the transmission peak in frequency.

18. The device as in claim 16, wherein each of the first and second optical resonators is a tunable electro-optic optical resonator.

19. The device as in claim 14, wherein the first optical resonator is a tunable electro-optic optical resonator.

20. The device as in claim 14, wherein the first and second optical resonators are not directly optically coupled to each other and are optically coupled via optical coupling to the first and second waveguides.

21. The device as in claim 14, wherein the first and second optical resonators are directly optically coupled to each other in addition to optical coupling with each other via optical coupling to the first and second waveguides.

22. The device as in claim 21, wherein the first and second optical resonators are directly coupled to make the transmission peak a third-order filter function.

23. The device as in claim 14, further comprising at least a third optical resonator with a third resonance frequency optically coupled to the first and second optical waveguides to cause an optical interference with optical signals that transmit through the first, second, and third optical resonators via the first and second waveguides.

24. The device as in claim 14, wherein the tuning mechanism operates to tune the first optical resonator to change a sum of the first and second resonance frequencies and to tune the transmission peak in frequency.

25. The device as in claim 14, wherein the first optical resonator is mechanically tunable.

26. The device as in claim 14, wherein the first optical resonator is optically tunable.

27. The device as in claim 14, wherein the first optical resonator is thermally tunable.

28. The device as in claim 14, wherein the first optical resonator is electrically tunable.

29. A device, comprising:

a first resonator in resonance with electromagnetic radiation at a first resonance frequency that is tunable to change the first resonance frequency;

a first waveguide coupled to the first optical resonator to exchange electromagnetic radiation;

a second waveguide coupled to the first resonator to exchange electromagnetic radiation;

a second resonator in resonance with electromagnetic radiation with a second resonance frequency and coupled to the first and second waveguides, respectively, to cause an electromagnetic interference between electromagnetic signals that transmit through the first and second resonators via the first and second waveguides to produce a narrow spectral transmission peak centered at an average frequency of the first and the second resonance frequencies; and

a tuning mechanism to tune the first resonator to change a difference between the first and second resonance frequencies to change a delay of electromagnetic radiation in the transmission peak.

30. The device as in claim 29, wherein the first and second resonators and waveguides are devices for microwave signals.

31. The device as in claim 29, wherein the first and second resonators and waveguides are devices for millimeter wave signals.

32. The device as in claim 29, wherein the first and second resonators and waveguides are devices for optical signals.

33. The device as in claim 29, wherein the first and second resonators are directly coupled to each other to exchange energy.

34. The device as in claim 29, further comprising a coupling element coupled between the first and second resonators to assist coupling of energy therebetween without going through the first and second waveguides.

35. A device, comprising:

a first optical resonator with a first resonance frequency;

a first optical waveguide optically coupled to the first optical resonator;

a second optical waveguide optically coupled to the first optical resonator;

a second optical resonator with a second resonance frequency and optically coupled to the first and second optical waveguides, respectively, to cause an optical interference between optical signals that transmit through the first and second optical resonators via the first and second waveguides to produce a narrow spectral transmission peak centered at an average frequency of the first and the second resonance frequencies,

wherein the first and second optical resonators are directly optically coupled to each other in addition to optical coupling with each other via optical coupling to the first and second waveguides.

36. The device as in claim 35, wherein at least the first optical resonator is tunable to change the first resonance frequency.

37. A device, comprising first, second, third, and fourth optical resonators optically coupled to one another in a configuration that,

the first optical resonator is optically coupled to the second and third optical resonators,

the second optical resonator is further optically coupled to the fourth optical resonator,

the third optical resonator is further optically coupled to the fourth optical resonator, and

the second and third optical resonators are not directly coupled to each other and are indirectly coupled via the first and fourth optical resonators.

38. The device as in claim 37, wherein at least one of the first, second, third, and fourth optical resonators is tunable to change a resonance frequency.

39. The device as in claim 37, further comprising:

a first optical coupler optically coupled to the first optical resonator to direct an input optical signal to the first optical resonator; and

a second optical coupler optically coupled to the fourth optical resonator to couple light in the fourth optical resonator out as an optical output signal.

40. The device as in claim 37, wherein the first and fourth optical resonators are half disk resonators and the second and third resonators are full disk resonators.