Stabilizing RF oscillator based on optical resonator

• US 8,804,231 B2
• Filed: 06/20/2012
• Issued: 08/12/2014
• Est. Priority Date: 06/20/2011
• Status: Active Grant

• Current Assignee: Oewaves Incorporated
• Original Assignee: Oewaves Incorporated
• Inventors: Savchenkov, Anatoliy A., Matsko, Andrey B., Maleki, Lute, Seidel, David, Ilchenko, Vladimir S.
• Primary Examiner(s): Hellner, Mark
• Assistant Examiner(s): Diacou, Ari M
• Application Number:
  US13/528,775
• Publication Number:
  US 20120320449A1
• Time in Patent Office: 783 Days
• US Class Current: 359/337.1
• CPC Class Codes: G02B 6/29341 Loop resonators operating in a whispering gallery mode evanescently coupled to a light guide, e.g. sphere or disk or cylinder evanescent coupling for sensing fluorescence G01N21/648
• CPC Class Codes: H01S 3/10092 Coherent seed, e.g. injection locking
• CPC Class Codes: H01S 3/1304 by using an active reference, e.g. second laser, klystron or other standard frequency source H01S3/139 takes precedence; automatic control of electronic generators H03L7/00
• CPC Class Codes: H01S 3/1305 Feedback control systems
• CPC Class Codes: H01S 5/0687 Stabilising the frequency of the laser

Abstract

Techniques, devices and systems that stabilize an RF oscillator by using an optical resonator that is stabilized relative to a master RF oscillator with acceptable frequency stability performance. In the examples described, the optical resonator is stabilized relative to the master RF oscillator by using a frequency stability indicator based on two different optical modes of the optical resonator. The RF oscillator to be stabilized is then locked to the stabilized optical resonator to achieve the acceptable RF stability in the RF oscillator.

Claims

1. A method for stabilizing a radio frequency (RF) oscillator of interest via an optical resonator stabilized to a master RF oscillator, comprising:

providing an optical resonator that is structured to support a first family of first optical modes and a second, different family of second optical modes, an optical mode in the first family and an optical mode in the second family exhibiting different susceptibilities to one or more external conditions of the optical resonator;

selecting a first optical mode in the first family at a first optical frequency and a second optical mode in the second family at a second, different optical frequency to generate a frequency difference between the first optical frequency of the selected first optical mode and the selected second optical mode at the second optical frequency as an indicator of a stability of the optical resonator with respect to the one or more external conditions;

monitoring an optical signal from the optical resonator that represents a change in the frequency difference between the first optical frequency and the second optical frequency;

stabilizing the optical resonator to reduce the monitored change in the frequency difference between the first optical frequency and the second optical frequency to stabilize the optical resonator with respect to a master RF frequency from a master RF oscillator; and

using information in the optical signal from the optical resonator to operate a locking circuit of an RF oscillator to lock an RF frequency of the RF oscillator of interest with respect to the optical resonator so that the RF oscillator of interest is stabilized relative to the master RF oscillator via the optical resonator.

2. The method as in claim 1, wherein:

the optical resonator exhibits optical birefringence and supports the first family of first optical modes in an ordinarily polarized mode and the second family of second optical modes in an extraordinarily polarized mode so that the selected first optical mode and the selected second optical mode experience different refractive indices and different responses to a change in temperature of the optical resonator.

3. The method as in claim 2, comprising:

using the frequency difference between the first optical frequency and the second optical frequency to monitor a change in temperature of the optical resonator without directly measuring the temperature of the optical resonator by using one or more temperature sensors.

4. The method as in claim 1, wherein the optical resonator is a monolithic resonator.

5. The method as in claim 1, wherein the optical resonator is a monolithic ring resonator.

6. The method as in claim 1, wherein:

the optical resonator is a whispering gallery mode resonator and the first family of first optical modes and the second family of second optical modes are whispering gallery modes.

7. The method as in claim 1, wherein the optical resonator is integrated on a planar semiconductor structure.

8. The method as in claim 1, comprising:

operating a laser to direct laser light into one mode of the optical resonator;

modulating the laser light inside the optical resonator to produce an optical harmonic to be coupled to the selected second optical mode of the optical resonator;

coupling the modulated light of the selected first optical mode and the selected second optical mode out of the optical resonator as the optical signal;

directing the optical signal into a photodetector to produce a detector signal containing information on the frequency difference; and

using the detector signal to lock the optical resonator to the master RF oscillator.

9. The method as in claim 8, comprising:

locking the laser to a selected optical mode of the optical resonator via optical feedback from the optical resonator to the laser.

10. The method as in claim 8, comprising:

locking the laser to the optical resonator via a Pound-Drever-Hall circuit.

11. The method as in claim 1, comprising:

in locking the RF oscillator of interest with respect to the optical resonator, selecting two optical modes at two different frequencies belonging to the same mode family from the first and second families to produce the information in the optical signal from the optical resonator by using a frequency difference between the two selected optical modes of the same family; and

using the frequency difference between the two selected optical modes of the same family as a frequency reference to lock the RF oscillator with respect to the optical resonator.

12. The method as in claim 1, wherein:

the one or more external conditions include a mechanical pressure applied to the optical resonator, a voltage applied to the optical resonator, or a temperature of a surrounding environment of the optical resonator.

17. The system as in claim 11, wherein:

the laser is locked to the optical resonator.

13. A system for stabilizing a radio frequency (RF) oscillator of interest via an optical resonator locked to a master oscillator, comprising:

a laser that produces laser light;

an optical resonator that is structured to support a first family of first optical modes and a second, different family of second optical modes, an optical mode in the first family and an optical mode in the second family exhibiting different susceptibilities to one or more external conditions of the optical resonator, the optical resonator being optically coupled to receive the laser light from the laser and to support the laser light inside the optical resonator at a selected first optical mode in the first family at a first optical frequency and a selected second optical mode in the second family at a second, different optical frequency, wherein a frequency difference between the first optical frequency of the selected first optical mode and the selected second optical mode at the second optical frequency indicates a stability of the optical resonator with respect to the one or more external conditions;

a photodetector that is coupled to receive an optical signal from the optical resonator that contains light in the selected first and second optical modes and produces a detector signal that represents a change in the frequency difference between the first optical frequency and the second optical frequency;

a master oscillator that produces a stable master oscillation signal;

an RF oscillator that produces an RF oscillation signal;

a first locking circuit coupled between the master oscillator and the optical resonator and operable to control the optical resonator to reduce the monitored change in the frequency difference between the first optical frequency and the second optical frequency and to stabilize the optical resonator with respect to the master oscillator; and

a second locking circuit coupled between the RF oscillator and the optical resonator and operable to control the RF oscillator to stabilize the RF oscillator relative to the optical resonator to lock an RF frequency of the RF oscillator with respect to the master oscillator via the optical resonator.

14. The system as in claim 13, wherein:

the optical resonator exhibits optical birefringence and supports the first family of first optical modes in an ordinarily polarized mode and the second family of second optical modes in an extraordinarily polarized mode so that the selected first optical mode and the selected second optical mode experience different refractive indices and different responses to a change in temperature of the optical resonator.

15. The system as in claim 14, wherein:

the optical resonator is a whispering gallery mode resonator and the first family of first optical modes and the second family of second optical modes are whispering gallery modes.

16. The system as in claim 15, wherein the master oscillator is an RF oscillator, and the system comprises:

an optical modulation mechanism that causes optical modulation of the laser light coupled into the optical resonator based on the stable mater oscillation signal from the master oscillator.

18. The system as in claim 13, wherein:

at least one of the first and second locking circuits is a Pound-Driver-Hall circuit.

19. The system as in claim 13, wherein:

the second locking circuit uses a frequency difference between two optical modes at two different frequencies of a same family from the first and second families as a frequency reference to lock the RF oscillator with respect to the optical resonator.

20. The system as in claim 13, wherein:

the one or more external conditions include a mechanical pressure applied to the optical resonator, a voltage applied to the optical resonator, or a temperature of a surrounding environment of the optical resonator.

21. The system as in claim 13, wherein:

the master oscillator is an optical oscillator.

22. The system as in claim 13, wherein:

the master oscillator is an RF oscillator that includes one or more opto-electronic oscillation loops.

23. A system for stabilizing a radio frequency (RF) oscillator with respect to an optical resonator, comprising:

a laser that produces laser light;

an optical resonator that is an optical whispering gallery mode resonator supporting a first family of first optical modes and a second, different family of second optical modes, wherein the optical resonator is structured so that an optical mode in the first family and an optical mode in the second family exhibit different susceptibilities to one or more external conditions of the optical resonator;

an optical coupler that couples the laser light into the optical resonator so the laser light inside the optical resonator is at a selected first optical mode in the first family at a first optical frequency and a selected second optical mode in the second family at a second, different optical frequency, wherein a frequency difference between the first optical frequency of the selected first optical mode and the selected second optical mode at the second optical frequency indicates a stability of the optical resonator with respect to the one or more external conditions;

a photodetector that is coupled to receive an optical signal from the optical resonator that contains light in the selected first and second optical modes and produces a detector signal that represents a change in the frequency difference between the first optical frequency and the second optical frequency;

a master RF oscillator that produces a stable master RF oscillation signal which is coupled to cause a first optical modulation in the laser light inside the optical resonator;

a first locking circuit coupled to receive the RF oscillation signal from the master RF oscillator and the detector signal from the photodetector and operable to control the optical resonator, based on the first optical modulation, to reduce the monitored change in the frequency difference between the first optical frequency and the second optical frequency and to stabilize the optical resonator with respect to the master RF oscillator;

an RF oscillator that produces an RF oscillation signal which is coupled to cause a second optical modulation in the laser light inside the optical resonator; and

a second locking circuit coupled between the RF oscillator and the optical resonator and operable to control, based on the second optical modulation, the RF oscillator to stabilize the RF oscillator relative to the optical resonator.

24. The system as in claim 23, wherein:

the laser is locked in frequency to an optical mode of the optical resonator.

25. The system as in claim 23, wherein:

the optical resonator is structured so that two different optical modes in the same family of optical modes and exhibit similar or the same susceptibilities to one or more external conditions of the optical resonator; and

the second locking circuit is configured to use a frequency difference between the two different optical modes of the same family to stabilize the RF oscillator relative to the optical resonator.