Method and system for generating a broadband spectral continuum and continuous wave-generating system utilizing same

• US 6,381,391 B1
• Filed: 12/03/1999
• Issued: 04/30/2002
• Est. Priority Date: 02/19/1999
• Status: Expired due to Fees

• Current Assignee: Board of Regents of the University of Michigan (University of Michigan)
• Original Assignee: Board of Regents of the University of Michigan (University of Michigan)
• Inventors: Islam, Mohammed N., Kim, Jaeyoun, Boyraz, Ozdal
• Primary Examiner(s): Ullah, Akm E.
• Application Number:
  US09/454,106
• Time in Patent Office: 879 Days
• Field of Search: 385/123-129, 385/147, 359/134, 359/161, 359/337, 359/160, 372/6, 372/8, 372/25, 623/45
• US Class Current: 385/123
• CPC Class Codes: G02B 6/274 based on light guide birefringence, e.g. due to coupling between light guides G02B6/105, G02B6/024 take precedence; mechanically induced birefringence G02F1/0134
• CPC Class Codes: G02B 6/2766 Manipulating the plane of polarisation from one input polarisation to another output polarisation, e.g. polarisation rotators, linear to circular polarisation converters
• CPC Class Codes: G02B 6/29376 coupling light guides for controlling wavelength dispersion, e.g. by concatenation of two light guides having different dispersion properties dispersion managed optical transmission systems H04B10/25253
• CPC Class Codes: G02F 1/3513 Soliton propagation
• CPC Class Codes: H04B 10/25077 using soliton propagation
• CPC Class Codes: H04B 10/506 Multiwavelength transmitters

Abstract

Method and system are disclosed for stable, multi-wavelength continuous wave (CW) generation using fiber-based supercontinuum and spectrum-slicing of its longitudinal modes. The continuum generated is coherent and stable, making it an attractive alternative as a spectrally-sliced source for continuous, multiple wavelength channels. A 140 nm wide supercontinuum with a 10 GHz repetition rate is generated in <30 meters of fiber. To obtain CW channels with 40 GHz spacing, time-domain multiplexing and longitudinal mode slicing are utilized. To obtain stable, continuous wave operation, short-fiber supercontinuum generation and a pulse interleaving method are utilized. The invention may be utilized as a broadband wavelength-division multiplexed source.

Claims

1. A method for generating a broadband spectral continuum, the method comprising the steps of:

generating soliton pulses at a repetition rate greater than or equal to 1 Gb/s;

compressing the higher-order soliton pulses in a temporal domain through soliton-effect compression to obtain compressed soliton pulses having a spectrum; and

breaking up the compressed soliton pulses to shape the spectrum of the compressed soliton pulses through higher order dispersion effects and self-phase modulation to obtain the broadband spectral continuum, the continuum having a plurality of substantially uniform longitudinal modes each of which is a narrow band continuous wave in the time domain and wherein the modes are spectrally spaced based on the repetition rate.

2. The method as claimed in claim 1 wherein the step of compressing includes the step of launching the higher-order soliton pulse into a first end of an anomalous dispersion fiber including at least one pulse compression stage having a length based on the order of the soliton pulse and a spectral shaping stage.

3. The method as claimed in claim 2 wherein the step of breaking up is performed adjacent a second end of the anomalous dispersion fiber in the spectral shaping stage.

4. The method as claimed in claim 3 wherein the spectral shaping stage is a dispersion-shifted optical fiber section of the anomalous dispersion fiber.

5. The method as claimed in claim 2 wherein the step of compressing is performed in multiple pulse compression stages of the anomalous dispersion fiber.

6. The method as claimed in claim 3 wherein the higher order dispersion effects include third order dispersion effects.

7. The method as claimed in claim 6 wherein the shape of the broadband spectral continuum is based primarily on the sign and magnitude of third order dispersion of the spectral shaping stage adjacent the second end.

8. The method as claimed in claim 7 wherein the shape of the broadband spectral continuum is also based on pulse width of the compressed soliton pulse immediately prior to the step of breaking up.

9. The method as claimed in claim 8 wherein the dispersion effects include second and third order dispersion effects, and wherein the magnitude of the second order dispersion and the magnitude of the third order dispersion normalized by the pulse width have substantially the same order of magnitude adjacent the second end of the anomalous dispersion fiber in the spectral shaping stage.

10. The method as claimed in claim 1 wherein the spectral continuum is greater than 15 nm wide.

11. A system for generating broadband spectral continuum, the system comprising:

a soliton pulse generator including a single laser for generating soliton pulses at a repetition rate greater than or equal to 1 Gb/s; and

an optical fiber including at least one pulse compression stage for compressing the soliton pulses through soliton-effect compression to obtain compressed soliton pulses having a spectrum, the optical fiber further including a spectral shaping stage optically coupled to the at least one pulse compression stage for breaking up the compressed soliton pulses adjacent an output end of the fiber to shape the spectrum of the compressed soliton pulses through higher order dispersion effects and self-phase modulation to obtain the broadband spectral continuum, the continuum having a plurality of substantially uniform longitudinal modes each of which is a narrow band continuous wave in the time domain and wherein the modes are spectrally spaced based on the repetition rate.

12. The system as claimed in claim 11 wherein the at least one pulse compression stage of anomalous dispersion fiber has a dispersion which is relatively constant therein.

13. The system as claimed in claim 11 wherein the anomalous dispersion fiber has a second pulse compression stage less than 100 meters in length.

14. The system as claimed in claim 13 wherein the second pulse compression stage is less than 30 meters in length.

15. The system as claimed in claim 11 wherein the dispersion effects include third order dispersions having a sign and a magnitude.

16. The system as claimed in claim 15 wherein the third order dispersions have a positive sign.

17. The system as claimed in claim 15 wherein the third order dispersions have a negative sign.

18. The system as claimed in claim 11 further comprising a plurality of pulse compression stages of anomalous dispersion fiber for compressing the soliton pulses through soliton-effect compression to obtain the compressed soliton pulses.

19. The system as claimed in claim 11 wherein the length of the at least one pulse compression stage of anomalous dispersion fiber is based on a minimal width of the compressed soliton pulses.

37. The invention as claimed in claims 2 or 11 wherein the fiber includes a high nonlinearity fiber.

38. The invention as claimed in claims 2 or 11 wherein the fiber includes a polarization preserving fiber.

39. The invention as claimed in claims 2 or 11 wherein the fiber includes a dispersion decreasing fiber.

20. A system for generating narrow band, continuous waves (CW) substantially simultaneously on multiple CW channels at multiple wavelengths and with channel spacing of at least 1 GHz, the system comprising:

a soliton pulse generator including a single laser for generating soliton pulses at a repetition rate greater than or equal to 1 Gb/s;

an optical fiber including at least one pulse compression stage and a spectral shaping stage, the at least one pulse compression stage receiving the soliton pulses at a first end of the fiber and the spectral shaping stage generating a broadband spectral continuum within the fiber and providing the broadband spectral continuum at a second end of the fiber, the continuum having a plurality of substantially uniform longitudinal modes each of which is a narrow band continuous wave in the time domain and wherein the modes are spectrally spaced based on the repetition rate; and

at least one optical filter coupled to the second end of the fiber for spectrally-slicing the longitudinal modes from the broadband spectral continuum to obtain the continuous waves.

21. The system as claimed in claim 20 further comprising a time domain multiplexer to adjust the spacing between the longitudinal modes.

22. The system as claimed in claim 21 wherein the multiplexer includes a pulse interleaver to increase channel spacing.

23. The system as claimed in claim 20 wherein the single laser is a single mode-locked laser.

24. The system as claimed in claim 23 wherein the single mode-locked laser is a mode-locked erbium-doped fiber laser.

25. The system as claimed in claim 20 wherein the single laser is a single continuous-wave (CW) laser adapted to be externally modulated.

26. The system as claimed in claim 23 wherein the single mode-locked laser is a mode-locked semiconductor laser.

27. The system as claimed in claim 20 wherein the at least one optical filter includes a monochromator, a Fabry-Perot, an arrayed wave guide grating, a Mach-Zehnder, or fused-tapered couplers.

28. The system as claimed in claim 20 wherein the length of the spectral shaping stage is less than 10 meters.

29. The system as claimed in claim 20 wherein the spectral shaping stage is a dispersion-shifted fiber.

30. The system as claimed in claim 20 wherein the optical fiber includes a polarization preserving fiber.

31. The system as claimed in claim 20 wherein the spectral continuum is greater than 15 nm wide.

32. The system as claimed in claim 20 wherein the soliton pulse generator includes a polarization controller for aligning polarization of the soliton pulses with a polarization eigenmode of the at least one pulse compression stage.

33. The system as claimed in claim 20 wherein the soliton pulse generator includes a fiber amplifier for amplifying the soliton pulses.

34. The system as claimed in claim 20 wherein the soliton pulse generator includes a semiconductor optical amplifier for amplifying the soliton pulses.

35. The system as claimed in claim 33 wherein the fiber amplifier is an erbium-doped fiber amplifier.

36. The system as claimed in claim 20 wherein the optical fiber includes a high-nonlinearity (Hi-NL) fiber.