IP Library › Granted Patent US 12,300,963
Granted Patent B2
US 12,300,963 · App. 17/400,813 · Granted May 13, 2025

Tunable optical frequency comb generator in microresonators

Inventors: Yoshitomo Okawachi (River Edge, NJ); Jae Jang (New York, NY); Xingchen Ji (New York, NY); Michal Lipson (New York, NY); Alexander L. Gaeta (New York, NY); Bok Young Kim (New York, NY)
Assignee: The Trustees of Columbia University in the City of New York
H01S5/005G02F1/015G02F1/212G02F2203/15G02F2203/56
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Quick Facts
Patent No.
US 12,300,963
App. No.
17/400,813
Granted
May 13, 2025
Kind
B2
Abstract

Optical frequency combs and related methods, devices, and systems are described. An example device can comprise a waveguide configured to optically couple to an optical source and at least one optical resonator optically coupled to the waveguide. The one or more of the at least one optical resonator can be tuned such that an optical frequency comb is generated based on mode interaction between two different modes of the at least one optical resonator. The device can comprise an output coupled to the waveguide and configured to output the optical frequency comb.

Claims (30)

1. A device, comprising:

a waveguide configured to optically couple to a single-frequency continuous wave optical source;

at least one optical resonator optically coupled to the waveguide, wherein one or more of the at least one optical resonator is tuned such that an optical signal supplied to the at least one optical resonator via the waveguide from the single-frequency continuous wave optical source causes generation of an optical frequency comb based on mode interaction between two different modes of the at least one optical resonator; and

an output coupled to the waveguide and configured to output the optical frequency comb.

2. The device of claim 1 , wherein the two different modes comprise (1) two spatial modes, (2) two polarization modes, (3) modes of two different resonators that are optically coupled, or (4) any combination thereof.

3. The device of claim 1 , wherein a bandwidth of the optical frequency comb is controlled by controlling of a coupling strength.

4. The device of claim 1 , wherein the device is comprised in one or more of an optical clock, molecular spectroscopy device, an astronomical spectrometer, a distance ranging device, or microwave generator device.

5. The device of claim 1 , wherein a coupling strength of the two different modes is controlled by adjusting a distance of an interaction between two optical resonators of the at least one optical resonator.

6. The device of claim 5 , wherein a wavelength at which the interaction occurs is tuned by adjusting a spectral position of a resonance.

7. The device of claim 1 , further comprising a PIN junction configured to electrically tune through free-carriers one or more of the at least one optical resonator, wherein the PIN junction comprises an indirect bandgap comprising or more silicon, germanium, or a combination thereof.

8. The device of claim 1 , wherein the device is comprised in a wavelength division multiplexing (WDM) system.

9. The device of claim 1 , wherein a bandwidth of the optical frequency comb is tune based on (1) a coupling strength between two different optical resonators of the at least one optical resonator, (2) a group velocity dispersion of the at least one optical resonator, or (3) any combination thereof.

10. The device of claim 1 , wherein the at least one optical resonator is tuned to control 1) a spectral position of a resonance of the at least one optical resonator, 2) dispersion of at least one optical resonator, or 3) a combination thereof.

11. A method, comprising:

supplying, from a single-frequency continuous wave optical source, an optical signal to at least one optical resonator;

tuning the at least one optical resonator to cause output, based on the optical signal, of an optical frequency comb, wherein the optical frequency comb is generated from the optical signal based on mode interaction between two different modes of the at least one optical resonator; and

outputting the optical frequency comb.

12. The method of claim 11 , wherein the two different modes comprise (1) two spatial modes, (2) two polarization modes, (3) modes of two different resonators that are optically coupled, or (4) any combination thereof.

13. The method of claim 11 , wherein tuning the at least one optical resonator comprises modifying a coupling strength of one or more of the at least one optical resonator to control a bandwidth of the optical frequency comb.

14. The method of claim 11 , wherein a coupling strength of the two different modes is controlled by adjusting a distance of an interaction between two optical resonators of the at least one optical resonator.

15. The method of claim 14 , wherein tuning the at least one optical resonator to cause output of an optical frequency comb comprises adjusting a spectral position of a resonance of one or more of the at least one optical resonator to tune a wavelength at which the interaction occurs.

16. The method of claim 11 , wherein tuning the at least one optical resonator to cause output of an optical frequency comb comprises adjusting a coupling strength of the two different modes using a Mach-Zehnder interferometer.

17. The method of claim 11 , wherein tuning the at least one optical resonator to cause output of an optical frequency comb comprises electrically tuning through free-carriers one or more of the at least one optical resonator using a PIN junction, wherein the PIN junction comprises an indirect bandgap comprising or more silicon, germanium, or a combination thereof.

18. The method of claim 11 , performing wavelength division multiplexing with the output optical frequency comb.

19. The method of claim 11 , wherein tuning the at least one optical resonator to cause output of an optical frequency comb comprises tuning a bandwidth of the optical frequency comb is tuned based on (1) a coupling strength between two different optical resonators of the at least one optical resonator, (2) a group velocity dispersion of the at least one optical resonator, or (3) any combination thereof.

20. The method of claim 11 , wherein tuning the at least one optical resonator to cause output of an optical frequency comb comprises controlling (1) a spectral position of a resonance of the at least one optical resonator, (2) dispersion of at least one optical resonator, or (3) any combination thereof.

21. The device of claim 1 , wherein the device is configured to cause a blue shift to adjust one or more of a mode interaction point or an optical resonance of one or more of the at least one optical resonator to cause one or more of stabilization or modelocking of the optical frequency comb.

22. The device of claim 1 , wherein the at least one optical resonator is tuned such that the optical frequency comb is modelocked.

23. The method of claim 11 , wherein tuning the at least one optical resonator comprises causing a blue shift to adjust one or more of a mode interaction point or an optical resonance of one or more of the at least one optical resonator to cause one or more of stabilization or modelocking of the optical frequency comb.

24. The method of claim 11 , wherein tuning the at least one optical resonator comprises tuning the optical frequency comb to be modelocked.

Assignments (2)
CONFIRMATORY LICENSE Recorded Feb 15, 2024
From: COLUMBIA UNIV. NEW YORK MORNINGSIDE
To: US DEPARTMENT OF ENERGY
Reel/Frame 066601/0537 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Mar 2, 2023
From: OKAWACHI, YOSHITOMO; JANG, JAE; JI, XINGCHEN; LIPSON, MICHAL; GAETA, ALEXANDER L.; KIM, BOK YOUNG
To: THE TRUSTEES OF COLUMBIA UNIVERSITY IN THE CITY OF NEW YORK
Reel/Frame 062856/0124 →
Continuity (3)
Continuation PCTUS2020017955 · Feb 12, 2020
Provisional Application 62804613 · Feb 12, 2019
Related Publication 20210373362A1 · Dec 2, 2021
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