Single and multiple soliton generation device and method

• US 10,270,529 B2
• Filed: 01/16/2017
• Issued: 04/23/2019
• Est. Priority Date: 01/16/2017
• Status: Active Grant

• Current Assignee: Ecole polytechnique fãdãrale de lausanne epfl (Schweizerische Eidgenossenschaft)
• Original Assignee: Ecole polytechnique fãdãrale de lausanne epfl (Schweizerische Eidgenossenschaft)
• Inventors: Karpov, Maxim, Brasch, Victor, Kippenberg, Tobias
• Primary Examiner(s): Wolf, Darren E
• Application Number:
  US15/406,811
• Publication Number:
  US 20180205463A1
• Time in Patent Office: 827 Days
• Field of Search: None
• CPC Class Codes: G02F 1/065 in an optical waveguide structure
• CPC Class Codes: G02F 1/073 specially adapted for gating or modulating in optical waveguides
• CPC Class Codes: G02F 1/3513 Soliton propagation
• CPC Class Codes: G02F 2203/26 Pulse shaping; Apparatus or methods therefor
• CPC Class Codes: G02F 2203/56 Frequency comb synthesizer
• CPC Class Codes: H04B 10/25077 using soliton propagation
• CPC Class Codes: H04B 10/40 Transceivers
• CPC Class Codes: H04B 10/50 Transmitters
• CPC Class Codes: H04B 10/508 Pulse generation, e.g. generation of solitons
• CPC Class Codes: H04B 10/60 Receivers

Abstract

A soliton generation apparatus comprising:

• • an optical resonator;
  • a pumping laser for providing light at a pumping wavelength into the optical resonator;
  • a generator for generating multiple solitons in the optical resonator;
  • a detuning device for changing the wavelength detuning between the pumping laser wavelength and an optical resonance wavelength of the optical resonator to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator.

Claims

1. A soliton generation apparatus comprising:

an optical resonator for generating multiple solitons;

a pumping laser for providing light at a pumping wavelength into the optical resonator;

a tuning device for tuning the pumping wavelength across an optical resonance wavelength of the optical resonator or the optical resonance wavelength of the optical resonator across the pumping wavelength to generate multiple solitons inside the optical resonator, and for changing the wavelength detuning between the pumping laser wavelength and the optical resonance wavelength of the optical resonator to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator;

a photodetector for receiving light output from the optical resonator and producing a corresponding output signal;

a processor configured to

control the tuning device to generate multiple solitons in the optical resonator and to change the wavelength detuning between the pumping laser wavelength and an optical resonance wavelength of the optical resonator to remove at least one soliton of the generated multiple solitons,

process the output signal to determine a removal of a soliton from the optical resonator through the identification of a step profile in the corresponding output signal,

stop detuning when the removal of the at least one soliton is determined from the corresponding output signal, and

control the detuning device to tune at a tuning speed slower than a thermal relaxation rate of the optical resonator.

2. Apparatus according to claim 1, wherein the detuning device comprises a thermal tuner configured to apply or remove thermal energy to or from the optical resonator to displace the optical resonance wavelength of the optical resonator towards the pumping wavelength.

3. Apparatus according to claim 2, wherein the thermal tuner is configured to apply or remove thermal energy to or from the optical resonator to displace the optical resonance wavelength of the optical resonator across the pumping wavelength to generate the multiple solitons in the optical resonator.

4. Apparatus according to claim 1, wherein

the pumping laser is configured to provide light at a first wavelength into the optical resonator;

and the apparatus includes;

a laser tuning controller configured to;

(a) forward tune the pumping laser to tune the pumping laser light from the first wavelength, across a cavity resonance of the optical resonator, to a second wavelength to generate a frequency comb and multiple solitons in the optical resonator, the second wavelength being longer than the first wavelength;

and configured to (b) backward tune the pumping laser light from the second wavelength to a third wavelength to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator, the third wavelength being shorter than the second wavelength.

5. Apparatus according to claim 4, wherein the processor is configured to determine the removal of a least one soliton during forward and/or backward tuning from the optical resonator light output signal.

6. Apparatus according to claim 5, wherein the processor is configured to control the laser tuning controller to stop tuning when the removal of a least one soliton is determined.

7. Apparatus according to claim 5, wherein the processor is configured to control the laser tuning controller to carry out further backward tuning until a single soliton remains in the optical resonator based on determined soliton removals.

8. Apparatus according to claim 5, wherein the processor is configured to control the laser tuning controller to backward tune the laser light from the second wavelength to the third wavelength to remove solely one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator.

9. Apparatus according to claim 5, wherein the processor is configured to control the laser tuning controller to backward tune the laser light from the third wavelength to lower wavelengths to remove solitons of the plurality of solitons one-by-one to provide a single soliton in the optical resonator.

10. Apparatus according to claim 5, wherein the processor is configured to control the laser tuning controller to adiabatically backward tune the laser light.

11. Apparatus according to claim 5, wherein the processor is configured to control the laser tuning controller to backward tune the laser light at a tuning speed that is slower than a thermal relaxation rate of the optical resonator.

12. Apparatus according to claim 1, wherein the optical resonator is a crystalline resonator or an on-chip resonator.

13. Apparatus according to claim 1, further including a phase modulator for modulating the pumping laser light to non-destructively probe soliton generation in the optical resonator.

14. Apparatus according to claim 13, further including a modulation response analyzer for receiving an optical response signal outputted by the optical resonator and configured to determine a modulation response signal representing the response of the optical resonator to the phase modulation of the pumping laser light.

15. Apparatus according to claim 14, further including a processor configured to determine, from the modulation response signal, an effective pump detuning value representing the detuning of the pump laser frequency/wavelength from a cavity resonance frequency/wavelength of the optical resonator during the apparatus operation or pumping.

16. Apparatus according to claim 15, wherein the processor is configured to monitor the effective pump detuning value to maintain a soliton state in the optical resonator.

17. Apparatus according to claim 16, wherein the processor is configured to adjust the effective pump detuning value by controlling the laser tuning controller to tune the pump laser frequency/wavelength to maintain a soliton state in the optical resonator.

18. Apparatus according to claim 14, further including a processor configured to monitor the evolution of the modulation response signal or the effective pump detuning value while carrying out backward tuning to determine the extinction of one single soliton state in the optical resonator.

19. Apparatus according to claim 18, wherein the processor is configured to monitor the evolution of the modulation response signal or the evolution of the effective pump detuning value during backward tuning to determine successive extinctions of individual solitons, and configured to control the laser tuning controller to stop tuning to provide a single soliton in the optical resonator.

20. Apparatus according to claim 19, wherein the processor is configured to monitor the effective pump detuning value and to control the tuning device or the laser tuning controller to tune the pump laser frequency/wavelength to maintain the single soliton state in the optical resonator.

21. Soliton generation apparatus according claim 1, wherein the optical resonator is a crystalline resonator or an on-chip resonator and the apparatus further includes a coupling waveguide optically coupled to the optical resonator, the pumping laser light being provided to the optical resonator via the coupling waveguide.

22. A soliton generation method including the steps of:

introducing pumping laser light at a pumping wavelength into an optical resonator;

generating multiple solitons in the optical resonator by tuning the pumping wavelength across an optical resonance wavelength of the optical resonator or tuning the optical resonance wavelength of the optical resonator across the pumping wavelength;

providing light output from the optical resonator to a photodetector to produce a corresponding output signal; and

changing the wavelength detuning between the pumping laser wavelength and the optical resonance wavelength of the optical resonator to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator, wherein the corresponding output signal is processed to determine a removal of a soliton from the optical resonator through the identification of a step profile in the corresponding output signal, and detuning is stopped when the removal of the at least one soliton is determined from the corresponding output signal to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator,

wherein the detuning device is tuned at a tuning speed slower than a thermal relaxation rate of the optical resonator.

23. Method according to claim 22, wherein the step of changing the wavelength detuning is carried out by applying or removing thermal energy to or from the optical resonator to displace the optical resonance wavelength of the optical resonator towards the pumping wavelength.

24. Method according to claim 22, wherein the step of generating multiple solitons is carried out by applying or removing thermal energy to or from the optical resonator to displace the optical resonance wavelength of the optical resonator across the pumping wavelength to generate the multiple solitons in the optical resonator.

25. Method according to claim 22 further including the steps of:

introducing the pumping laser light at a first wavelength into the optical resonator;

forward tuning the pumping laser light from the first wavelength, across theft cavity resonance of the optical resonator, to a second wavelength to generate a frequency comb and multiple solitons in the optical resonator, the second wavelength being longer than the first wavelength; and

backward tuning the pumping laser light from the second wavelength to a third wavelength to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator, the third wavelength being shorter than the second wavelength.

26. Method according to claim 25, wherein the step of backward tuning the laser light from the second wavelength to the third wavelength removes solely one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator.

27. Method according to claim 26, further including the step of backward tuning the laser light from the third wavelength to lower wavelengths to remove solitons of the plurality of solitons one-by-one to provide a single soliton in the optical resonator.

28. Method according to claim 25, wherein the backward tuning of the laser light is carried out adiabatically.

29. Method according to claim 25, wherein the backward tuning of the laser light is carried out at a tuning speed that is slower than a thermal relaxation rate of the optical resonator.

30. Method according to claim 25, wherein the backward tuning of the laser light is carried out at a constant tuning speed.

31. Method according to claim 25, wherein the intensity of the pumping laser light is substantially constant.

32. Method according to claim 25, wherein the soliton is a dissipative Kerr soliton and/or the optical resonator is a crystalline resonator or an on-chip resonator.

33. Method according to claim 22, further including the step of phase modulating the pumping laser light to non-destructively probe soliton generation in the optical resonator.

34. Method according to claim 33, further including the step of measuring an optical response signal outputted by the optical resonator and determining a modulation response signal to non-destructively probe soliton generation in the optical resonator.

35. Method according to claim 34, further including the step of determining, from the modulation response signal, an effective pump detuning value representing the detuning of the pump laser frequency/wavelength from they cavity resonance frequency/wavelength of the optical resonator during the apparatus operation or pumping.

36. Method according to claim 35, further including the step of monitoring the effective pump detuning value to maintain a soliton state in the optical resonator.

37. Method according to claim 36, further including the step of adjusting the effective pump detuning value by tuning the optical resonance wavelength of the optical resonator or the pump laser frequency/wavelength to maintain a soliton state in the optical resonator.

38. Method according to claim 34, further including the step of monitoring the evolution of the modulation response signal or the effective pump detuning value while carrying out backward tuning to determine the extinction of one single soliton state in the optical resonator.

39. Method according to claim 32, wherein monitoring of the modulation response signal or the evolution of the effective pump detuning value is carried out while carrying out backward tuning to determine successive extinctions of individual solitons and provide a single soliton in the optical resonator.

40. Method according to claim 39, further including the steps of monitoring and adjusting the effective pump detuning value to maintain the single soliton state in the optical resonator.