Fibre-grating-stabilized diode laser

• US 5,715,263 A
• Filed: 12/19/1995
• Issued: 02/03/1998
• Est. Priority Date: 06/28/1994
• Status: Expired due to Term

• Current Assignee: Viavi Solutions, Inc. (Lumentum Holdings Inc.)
• Original Assignee: SDL PLC (RWS Holdings Plc)
• Inventors: Rogers, Grant, Ventrudo, Brian F.
• Primary Examiner(s): Bovernick, Rodney B.
• Assistant Examiner(s): Song, Yisun
• Application Number:
  US08/575,705
• Time in Patent Office: 777 Days
• Field of Search: 372/6, 372/22, 372/29, 372/96, 372/99, 372/108, 372/102, 372/32, 385/2, 385/10, 385/28, 385/31, 385/33, 385/37
• US Class Current: 372/6
• CPC Class Codes: G02B 6/02057 comprising gratings
• CPC Class Codes: G02B 6/02076 Refractive index modulation gratings, e.g. Bragg gratings
• CPC Class Codes: H01S 2301/02 ASE (amplified spontaneous emission), noise; Reduction thereof
• CPC Class Codes: H01S 3/0826 using a diffraction grating
• CPC Class Codes: H01S 5/065 Mode locking; Mode suppression; Mode selection ; Self pulsating
• CPC Class Codes: H01S 5/0656 Seeding, i.e. an additional light input is provided for controlling the laser modes, for example by back-reflecting light from an external optical component H01S5/14, H01S5/4062 and H01S5/4006 take precedence
• CPC Class Codes: H01S 5/0657 Mode locking, i.e. generation of pulses at a frequency corresponding to a roundtrip in the cavity
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence
• CPC Class Codes: H01S 5/146 using a fiber as external cavity
• CPC Class Codes: H01S 5/4025 Array arrangements, e.g. constituted by discrete laser diodes or laser bar H01S5/42 takes precedence
• CPC Class Codes: H01S 5/4062 with an external cavity or using internal filters, e.g. Talbot filters

Abstract

A fibre Bragg grating is used to stabilize the intensity and frequency fluctuations of a diode laser. The diode laser is connected with an opto-mechanical apparatus to the fibre which contains the grating. The grating is formed in the guided-mode region of the optical fibre. The wavelength of maximum grating reflectivity is selected to lie near the maximum of the diode laser gain bandwidth. The magnitude and bandwidth of the grating reflectivity stabilizes the diode laser output without appreciably reducing the optical output power from the end of the fibre. The bandwidth of the optical spectrum of the diode laser is selected depending on the distance of the grating from the diode laser.

Claims

1. An optical feedback system comprising:

a gain medium having a first optical cavity and having an output;

at least a first reflecting component in said first optical cavity and having an output facet providing a first reflectivity level for reflecting a portion of propagating light in said first optical cavity back into said cavity, said facet also providing a light output;

an optical fibre optically coupled to said first cavity to receive said light output;

a reflective element accompanying said optical fibre, said reflective element having a supplemental reflectivity level for reflecting a portion of said output over a narrow band of wavelengths back into said first cavity;

said supplemental reflectivity level approximately equal to or less than said first reflectivity level;

said fibre reflective element positioned in said optical fibre an optical distance from said first optical cavity sufficient to induce multiple longitudinal mode operation of said gain medium to suppress longitudinal mode hoping.

2. The optical feedback system of claim 1 wherein said gain medium is a semiconductor laser having a gain band at least a portion of which overlaps with said reflectivity band.

3. The optical feedback system of claim 2 wherein said fibre is a single mode fibre.

5. The optical feedback system of claim 2 wherein said reflective element is positioned beyond the coherence length of said laser.

6. The optical feedback system of claim 2 wherein said overlap of the gain band and reflectivity band stabilizes the operational wavelength of said laser over a range of operating conditions.

7. The optical feedback system of claim 6 wherein at least one of said operating conditions is a change in ambient temperature.

8. The optical feedback system of claim 2 wherein said semiconductor laser has an InGaAs strained layer quantum well gain medium.

10. The optical feedback system of claim 8 wherein said reflective element is positioned beyond the coherence length of said laser.

13. The optical feedback system of claims 1 wherein said reflective element has a reflectivity peak which is within 10 nm of the peak gain of said gain medium.

14. The optical feedback system of claim 1 wherein said reflective element has a reflection bandwidth between about 0.05 nm and 2 nm.

15. The optical feedback system of claim 1 wherein said reflective element is a Bragg grating formed in said optical fibre.

4. An optical feedback system comprising:

a gain medium having a first optical cavity and having an output;

at least a first reflecting component in said first optical cavity and having a first reflectivity level;

an optical fibre optically coupled to said first cavity;

a reflective element accompanying said optical fibre, said reflective element having a supplemental reflectivity level for reflecting a portion of said output over a narrow band of wavelengths back into said first cavity;

said supplemental reflectivity level approximately equal to or less than said first reflectivity level;

said fibre grating positioned in said optical fibre an optical distance from said first optical cavity sufficient to induce multiple longitudinal mode operation of said gain medium;

said gain medium is a semiconductor laser having a gain band at least a portion of which overlaps with said reflectivity band;

said supplemental reflectivity level sufficient to induce coherence collapse in said laser.

11. The apparatus of claim 4 wherein said supplemental reflectivity level is less than said first reflectivity level but of sufficient magnitude to maintain said coherence collapse and greater than any extraneous feedback present in said fibre.

9. The optical feedback system of 8 wherein said reflective element has a reflectivity peak which is within 10 nm of the peak gain of said gain medium.

12. An optical feedback system comprising:

a gain medium having a first optical cavity and having an output;

at least a first reflecting component in said first optical cavity and having a first reflectivity level;

an optical fibre optically coupled to said first cavity;

a reflective element accompanying said optical fibre, said reflective element having a supplemental reflectivity level for reflecting a portion of said output over a narrow band of wavelengths back into said first cavity;

said supplemental reflectivity level approximately equal to or less than said first reflectivity level;

said fibre grating positioned in said optical fibre an optical distance from said first optical cavity sufficient to induce multiple longitudinal mode operation of said gain medium;

said gain medium is a semiconductor laser having a gain band at least a portion of which overlaps with said reflectivity band;

said supplemental reflectivity level about 2 to 3 times less than said first reflectivity level.

16. Apparatus for generating a stable laser source comprising:

a laser source having a lasing cavity and a light beam output at a laser facet, said laser facet also providing a level of partial reflectivity for a portion of said light beam in said laser cavity for optical feedback therein, said light beam output comprising a wavelength band of light dependent upon the instantaneous operating characteristics of said laser source;

an optical fibre having an input end coupled to said laser source to receive said light beam into said fibre;

a grating formed in said optical fibre, said grating having a reflectivity band for partially reflecting selected wavelengths defined by said reflectivity band back into said laser cavity;

the reflectivity level of said optical fiber grating being approximately equal to or less than the reflectivity level of said laser source facet;

said fibre grating is sufficiently spaced from said laser source to induce multiple longitudinal mode operation of said laser source for enhancing optical spectrum stability and intensity.

17. The apparatus of claim 16 wherein said laser source contains a strained layer InGaAs quantum well.

18. The apparatus of claim 16 wherein said fibre input end coupling comprises a lens.

19. The apparatus of claim 16 wherein said fibre input end coupling comprises close position of said input end relative to said laser source facet.

20. The apparatus of claim 16 wherein said grating has a maximum reflectivity within 10 nm of the emission wavelength of said laser source absent said grating.

21. The apparatus of claim 16 wherein the reflection bandwidth of said grating is between about 0.05 nm and 2 nm.

22. The apparatus of claim 16 wherein the wavelength of maximum reflectivity of said grating wavelength band is within the gain bandwidth of said laser source.

23. The apparatus of claim 16 wherein the effective reflectivity, R_eff of said grating is

24. The apparatus of claim 16 wherein the spacing of said grating from said fibre input end is greater than the coherence length of said light beam output.

25. Apparatus for generating a stable laser source comprising:

a laser source comprising a semiconductor laser having an output facet for reflecting a portion of propagating light in the laser cavity back into said cavity, said facet also providing a light output;

a bias current means for excitation of said laser to operate over a bias current range within a given temperature range;

an optical fiber optically coupled to receive said laser light output;

a grating in said optical fiber providing partial reflection over a narrow band of wavelengths, said wavelengths at least partially overlapping the wavelength emission band of said laser, said reflection providing optical feedback to said laser;

the bias current and temperature range of said laser and the reflectivity band of said grating selected so that said laser source operates in multiple longitudinal modes such that the longitudinal mode hopping noise of said laser source is reduced providing enhanced optical spectrum stability.

27. The apparatus of claim 25 wherein a reflection peak of said grating wavelength band is within 10 nm of an emission peak of said laser wavelength emission band absent said grating.

28. The apparatus of claim 25 said grating has a reflection bandwidth that is approximately equal to or less than 2 nm.

29. The apparatus of claim 25 wherein a spatial distance between said grating and said laser source output facet is longer than the coherence collapse distance of said laser.

30. The apparatus of claim 29 wherein said spatial distance is between about 50 centimeters and several meters.

31. The apparatus of claim 29 wherein said optical fiber has low birefringence so that it is polarization insensitive.

32. The apparatus of claim 31 wherein said optical fiber is polarization insensitive when stressed.

33. The apparatus of claim 25 wherein said optical fiber has a core doped with germanium, said grating is made by exposure of said fibre to UV light.

34. The apparatus of claim 25 wherein said optical fibre is coupled to another fibre via an optical coupler, said another fibre characterized by having an absorption band and capable of gain, said gain being produced by absorption of said output by said another fibre, the reflectivity peak and effective reflectivity of said grating selected to cause said laser to maintain a stable wavelength emission band of said output within the absorption band of said another fibre.

35. The apparatus of claim 25 wherein said grating stabilizes said laser wavelength emission band sufficiently to eliminate the need for active temperature control over the operating temperature range of said laser.

36. The apparatus of claim 25 wherein said laser operates with varying temperature and said grating provides optical feedback to stabilize the operation of said laser within a desired narrow range of wavelengths despite said temperature variation so that, in absence of said grating reflection, said operating wavelength would shift outside of said desired narrow range of wavelengths.

26. Apparatus for generating a stable laser source comprising:

a laser source comprising a semiconductor laser having an output facet for providing a light output;

a bias current means for excitation of said laser to operate over a bias current range within a given temperature range;

an optical fiber optically coupled to receive said laser light output;

a grating in said optical fiber providing partial reflection over a narrow band of wavelengths, said wavelengths at least partially overlapping the wavelength emission band of said laser, said reflection providing optical feedback to said laser;

the bias current and temperature range of said laser and the reflectivity band of said grating selected so that said laser source operates in multiple longitudinal modes such that the longitudinal mode hopping noise of said laser source is reduced;

the reflectivity of said grating is less than or equal to the reflectivity of said laser output facet.

37. Apparatus for generating a stable laser source comprising:

a laser source having an output facet providing optical feedback and for providing an output, said output optically coupled to an optical fibre;

a grating in said fibre providing a narrow wavelength band including wavelengths that are at least partially overlapping said wavelength emission spectrum of said laser source, absent said grating, and at least partially reflected to provide optical feedback to said laser source via said grating;

separation between said grating and laser source and magnitude of optical feedback from said grating being selected such that said laser source is constrained to operate at the peak wavelength of said grating and within the multiple longitudinal modes of the grating bandwidth so that longitudinal mode hopping of said laser source is suppressed.

38. The apparatus of claim 37 wherein the effective reflectivity of said grating is less than or equal to the effective reflectivity of reflective means provided integral with said laser source.

39. The apparatus of claim 37 said grating has a reflection bandwidth that is approximately equal to or less than 2 nm.

40. The apparatus of claim 37 wherein a spatial distance between said fiber grating and said laser source output facet is less than several meters.

41. The apparatus of claim 40 wherein said spatial distance is between about 50 centimeters and several meters.

42. The apparatus of claim 37 wherein a spatial distance between said fiber grating and said laser source is longer than the distance causing coherence collapse.

43. The apparatus of claim 37 wherein said optical fiber has low birefringence so that it is polarization insensitive.

44. The apparatus of claim 43 wherein said optical fiber is polarization insensitive when stressed.

45. The apparatus of claim 37 wherein said grating controls said output to be at a wavelength within an absorption band of a solid state gain medium.

46. The apparatus of claim 45 wherein said solid state gain medium includes a fibre amplifier.

47. The apparatus of claim 45 wherein said solid state gain medium includes a fibre laser.

59. The apparatus of claim 37 wherein the peak reflectivity of said grating being within 10 nm of said wavelength emission band of said laser source.

60. The apparatus of claim 37 wherein a reflectivity level of said grating is greater than extraneous feedback to said laser source.

48. Apparatus for generating a stable laser source comprising:

a laser source having a lasing cavity and a light beam output at a laser facet, said output optically coupled to an optical fibre;

a grating in said fibre such that a narrow band of wavelengths are reflected which at least partially overlaps a wavelength emission band of said laser source absent said grating;

a reflectivity level of said grating being approximately equal to or less than a reflectivity level of said laser source output facet with said fibre grating spaced from said laser source for enhancing optical spectrum stability and intensity.

49. The apparatus of claim 48 wherein a reflection peak of said grating wavelength band is within 10 nm of an emission peak of said laser wavelength emission band in the case where said grating is not present.

50. The apparatus of claim 48 wherein the effective reflectivity of said grating is less than or equal to the effective reflectivity of reflective means provided integral with said laser source.

51. The apparatus of claim 48 said grating has a reflection bandwidth that is approximately equal to or less than about 1 nm.

52. The apparatus of claim 48 wherein a spatial distance between said fiber grating and said laser source output facet is less than several meters.

53. The apparatus of claim 52 wherein said spatial distance is between about 50 centimeters and several meters.

54. The apparatus of claim 48 wherein said optical fiber has low birefringence so that it is polarization insensitive.

55. The apparatus of claim 54 wherein said optical fiber is polarization insensitive when stressed.

56. The apparatus of claim 48 wherein said grating controls said output to be at a wavelength within an absorption band of a solid state gain medium.

57. The apparatus of claim 56 wherein said solid state gain medium includes a fibre amplifier.

58. The apparatus of claim 56 wherein said solid state gain medium includes a fibre laser.

61. The apparatus of claim 48 wherein said grating is positioned in said fibre at or beyond the coherence length of said laser source.

62. The apparatus of claim 48 wherein a spatial distance between said grating and said laser source is sufficient to cause coherence collapse of said laser source.

63. The apparatus of claim 48 wherein said optical spectrum stability of said laser source is brought about, at least in part, by causing said laser source to operate in multiple longitudinal modes in a manner suppressing longitudinal mode hopping.