Amplitude and phase modulation of a laser by modulation of an output coupler

• US 8,917,748 B2
• Filed: 03/21/2011
• Issued: 12/23/2014
• Est. Priority Date: 03/19/2010
• Status: Active Grant

• Current Assignee: The Governing Council of the University of Toronto (University of Toronto), University of Toronto
• Original Assignee: The Governing Council of the University of Toronto (University of Toronto)
• Inventors: Poon, Joyce Kai See, Sacher, Wesley David
• Primary Examiner(s): Rodriguez, Armando
• Application Number:
  US13/634,295
• Publication Number:
  US 20120327961A1
• Time in Patent Office: 1,373 Days
• Field of Search: 372/26, 372/108
• US Class Current: 372/26
• CPC Class Codes: H01S 3/083 Ring lasers fibre ring lasers H01S3/06791
• CPC Class Codes: H01S 3/10038 Amplitude control
• CPC Class Codes: H01S 3/105 by controlling the mutual position or the reflecting properties of the reflectors of the cavity , e.g. by controlling the cavity lengthH01S3/10076, H01S3/13 take precedence
• CPC Class Codes: H01S 3/107 using electro-optic devices, e.g. exhibiting Pockels or Kerr effect H01S3/1061, H01S3/1063, H01S3/1065 take precedence
• CPC Class Codes: H04B 10/504 using direct modulation

Abstract

There is provided an output coupler modulated laser. The laser includes an optical resonator for light to circulate within, a gain medium housed within the optical resonator and a pump. An output coupler included in the optical resonator is responsive to a control signal to generate a modulated optical signal at a laser output port, and a complementary signal at a through port to retain circulating light within the optical resonator. The output coupler and the pump are jointly controllable to maintain the power level of the circulating light substantially at a selected, steady state level, and to decouple the modulation response of the laser from the intrinsic response of the circulating light due to interaction with the gain medium. The output coupler is configurable for simple amplitude modulation, Phase-Shift Keying (PSK), Quadrature Amplitude Modulation (QAM), and is suitable for use with high-finesse, micron or millimeter scale resonators.

Claims

1. A modulated laser comprising:

an optical resonator for light to circulate within;

a gain medium housed within the optical resonator in the path of the circulating light;

a pump for delivering excitation energy to the gain medium above a laser threshold of the optical resonator to bring the circulating light into coherent oscillation; and

an output coupler included in the optical resonator in the path of the circulating light, the output coupler responsive to a control signal to selectively allow a fraction of the circulating light to exit the optical resonator as a modulated optical signal, the output coupler having an input port to receive the circulating light into the output coupler, an output-coupled port to emit the modulated optical signal, and a through port complementary to the output-coupled port to retain unemitted light within the optical resonator.

2. The laser of claim 1, wherein the output coupler further comprises an interference section providing optical coupling between the input port and each of the output-coupled port and the through port, the interference section having an operating characteristic that is controllable by the control signal to provide selective optical interference in the interference section.

3. The laser of claim 2, wherein the operating characteristic of the interference section is controllable to generate the modulated optical signal at the output-coupled port and an optical signal complementary to the modulated optical signal at the through port.

4. The laser of claim 3, wherein the operating characteristic of the interference section is one of a refractive index and gain/attenuation.

5. The laser of claim 4, wherein the interference section of the output coupler is formed integrally with the optical resonator.

6. The laser of claim 1, wherein the output coupler comprises at least one Mach-Zehnder Interferometer (MZI).

7. The laser of claim 1, wherein the output coupler comprises at least one of a directional coupler, a multi-mode interference coupler, a waveguide junction and splitter, a Bragg reflector and a resonator, and wherein one of a refractive index and gain/attenuation of the output coupler is controllable by the control signal to generate the modulated optical signal.

8. The laser of claim 1, wherein the output coupler is responsive to the control signal to modulate at least one of amplitude and phase in the modulated optical signal.

9. The laser of claim 8, wherein the output coupler is responsive to the control signal applies at least one of an amplitude, a Phase-Shift Keying (PSK), and a Quadrature Amplitude Modulation (QAM) modulation scheme to the modulated optical signal.

10. The laser of claim 1, wherein the output coupler and pump are jointly controllable to decouple a modulation response of the laser from an intrinsic response of the circulating light due to interaction with the gain medium, the laser thereby substantially inheriting a modulation response of the output coupler.

11. The laser of claim 1, wherein the output coupler and pump are jointly controllable to maintain a power level of the circulating light within an operable range around a selected, steady-state power level.

12. The laser of claim 1, wherein the output coupler is controllable at a modulation rate selected to exceed a relaxation resonance frequency of the laser.

13. The laser of claim 1, wherein the output coupler is controllable to provide amplitude changes in a coefficient of output-coupling.

14. The laser of claim 1, wherein the pump is configured to deliver dc excitation energy to the gain medium.

15. The laser of claim 1, wherein the modulated output signal is free of chirp or has controllable chirp.

16. The laser of claim 1, further comprising at least one wavelength tuning section included in the optical resonator in the path of the circulating light, the wavelength tuning section selectively adjusting a refractive index or optical feedback of the optical resonator to control a wavelength of the modulated optical signal.

17. The laser of claim 1, wherein the optical resonator comprises a ring structure having opposite ends optically coupled with the input and through ports of the output coupler, the ring structure and output coupler defining a ring resonator for the circulating light.

18. The laser of claim 1, wherein the optical resonator further comprises a reflector optically coupled to each of the input port and through port of the output coupler, the reflectors creating a standing wave pattern for the circulating light.

19. The laser of claim 1, wherein the output coupler is formed monolithically on a semiconductor die.

20. The laser of claim 1, wherein the output coupler is integrated heterogeneously within the optical resonator.

21. The laser of claim 1, wherein the optical resonator is a high-finesse, micron or millimeter scale resonator.

22. A method of modulating a laser comprising an optical resonator for light to circulate within and a gain medium housed within the optical resonator in the path of the circulating light, the method comprising:

delivering excitation energy to the gain medium above a laser threshold of the optical resonator to bring the circulating light into coherent oscillation;

providing an output coupler in the optical resonator in the path of the circulating light;

determining a control signal for the output coupler, the output coupler responsive to the control signal to selectively allow a fraction of the circulating light to exit the optical resonator; and

controlling the output coupler using the control signal to generate a modulated optical signal by;

receiving the circulating light into an input port of the output coupler;

generating the modulated optical signal at an output-coupled port of the output coupler in response to the control signal; and

directing unemitted light to a through port of the output coupler to be retained within the optical resonator.

23. The method of claim 22, wherein an interference section provides optical coupling between the input port and each of the output-coupled port and the through port, and controlling the output coupler comprises controlling an operating characteristic of the interference section using the control signal to provide selective optical interference in the interference section.

24. The method of claim 23, wherein controlling the operating characteristic of the interference section generates the modulated optical signal at the output-coupled port and an optical signal complementary to the modulated optical signal at the through port.

25. The method of claim 24, wherein the operating characteristic of the interference section is one of a refractive index and gain/attenuation.

26. The method of claim 22, wherein controlling the output coupler comprises modulating at least one of amplitude and phase in the modulated optical signal.

27. The method of claim 26, wherein controlling the output coupler comprises applying at least one of an amplitude, a Phase-Shift Keying (PSK), and a Quadrature Amplitude Modulation (QAM) modulation scheme to the modulated optical signal.

28. The method of claim 22, further comprising jointly controlling the output coupler and the pump to decouple a modulation response of the laser from an intrinsic response of the circulating light due to interaction with the gain medium.

29. The method of claim 22, further comprising jointly controlling the output coupler and the pump to maintain a power level of the circulating light within an operable range around a selected, steady-state power level.

30. The method of claim 22, wherein controlling the output coupler comprises selecting a modulation rate that exceeds a relaxation resonance frequency of the laser and controlling the output coupler at the selected modulation rate.

31. The method of claim 22, wherein controlling the output coupler comprises controlling amplitude changes in a coefficient of output-coupling.

32. The method of claim 22, wherein the excitation energy comprises dc excitation energy.

33. The method of claim 22, wherein the modulated output signal is free of chirp or has controllable chirp.

34. The method of claim 22, wherein the method further comprises controlling a wavelength of the modulated optical signal by selectively adjusting a refractive index or optical feedback of the optical resonator using at least one wavelength tuning section included in the optical resonator in the path of the circulating light.