Integrated passively modelocked fiber lasers and method for constructing the same

US 6,072,811 A
Filed: 02/11/1998
Issued: 06/06/2000
Est. Priority Date: 02/11/1998
Status: Expired due to Term

First Claim

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1. A modelocked fiber laser, comprising:

a pump laser for generating laser energy at a pump wavelength;

a highly-birefringent fiber gain medium having first and second polarization axes and having first and second ends which respectively define first and second ends of a laser cavity for amplifying the laser energy at a signal wavelength;

a reflector coupled to the first end of said laser cavity, for reflecting the laser energy through said highly-birefringent fiber gain medium;

a saturable absorber coupled to the second end of said laser cavity, for inducing modelocking of said fiber laser along either of said first and second polarization axes of said highly-birefringent fiber gain medium in the absence of any non-fiber, intra-cavity, polarization-manipulating elements; and

an output for outputting the laser energy amplified within said laser cavity.

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Abstract

Stable operation of an ultra-compact modelocked fiber laser generating short optical pulses generally without use of any non-fiber, intra-cavity polarization-manipulating elements is obtained by employing a saturable absorber coupled to one end of a highly-birefringent fiber serving as the laser cavity. Once the laser is modelocked in one of the polarization axes of the highly-birefringent fiber, the degeneracy of the polarization axis is eliminated and cw oscillation along the other polarization axis is also prevented. Without a polarization-dependent loss in the cavity, the modelocked polarization axis is indeterminate, i.e., modelocking can occur on either of the polarization axes. However, the introduction of only a small polarization dependent loss is sufficient to ensure the reliable start-up of modelocking on only the low-loss axis. Such a small polarization dependent loss can be introduced by tightly coiling the highly-birefringent fiber, which generates a higher loss along the fast axis; thus, reliable modelocked operation along the slow axis is obtained. Alternatively, single polarization operation is obtained by employing a saturable absorber with a polarization-dependent loss or by introducing polarization-manipulating elements external to the laser cavity.

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63 Claims

1. A modelocked fiber laser, comprising:
- a pump laser for generating laser energy at a pump wavelength;
  
  a highly-birefringent fiber gain medium having first and second polarization axes and having first and second ends which respectively define first and second ends of a laser cavity for amplifying the laser energy at a signal wavelength;
  
  a reflector coupled to the first end of said laser cavity, for reflecting the laser energy through said highly-birefringent fiber gain medium;
  
  a saturable absorber coupled to the second end of said laser cavity, for inducing modelocking of said fiber laser along either of said first and second polarization axes of said highly-birefringent fiber gain medium in the absence of any non-fiber, intra-cavity, polarization-manipulating elements; and
  
  an output for outputting the laser energy amplified within said laser cavity.
- View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28, 29, 30, 31, 32, 33, 34, 35, 36, 37, 38, 39, 40, 41, 42, 43, 44, 45, 46, 47, 48, 49)
- - 2. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium includes a rare-earth-doped fiber.
  - 3. The modelocked fiber laser according to claim 2, wherein said rare-earth-doped fiber includes at least one of:
    - Er, Yb, Er/Yb, Nd, Pr, Ho and Tm.
  - 4. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium has a birefringence greater than 1.0×
    - 10^-5.
  - 5. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium has a birefringence which is due primarily to internal stresses inside said highly-birefringent fiber gain medium.
  - 6. The modelocked fiber laser according to claim 1, wherein the polarization axis of said highly-birefringent fiber gain medium along which modelocking occurs is indeterminate prior to application of the laser energy from said pump laser.
  - 7. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium is bent such that a loss differential exists between said first and second polarization axes, which loss differential causes modelocking to occur along a predetermined one of said first and second polarization axes.
  - 8. The modelocked fiber laser according to claim 7, wherein a portion of said highly-birefringent fiber gain medium is coiled with a coiling diameter between approximately 5 mm and 10 cm, and preferably between 12.5 mm and 10 cm.
  - 9. The modelocked fiber laser according to claim 7, wherein said highly-birefringent fiber gain medium is coherently bent such that an orientation of the first and second polarization axes is controlled with respect to a bend of said highly-birefringent fiber gain medium.
  - 10. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium has a D-shaped cross-section or a rectangular cross-section.
  - 11. The modelocked fiber laser according to claim 1, wherein said reflector comprises a dichroic mirror coupled to said pump laser, said dichroic mirror being at least partially transmissive at the pump wavelength such that the laser energy from said pump laser is transmitted into said laser cavity.
  - 12. The modelocked fiber laser according to claim 11, further comprising a pigtail fiber connecting said pump laser to said dichroic mirror.
  - 13. The modelocked fiber laser according to claim 12, wherein said output is coupled to said dichroic mirror, said dichroic mirror being partially transmissive at the signal wavelength, such that the amplified laser energy is transmitted from said laser cavity to said output.
  - 14. The modelocked fiber laser according to claim 13, wherein said pigtail fiber receives the laser energy at the pump wavelength from said pump laser and receives the amplifier laser energy at the signal wavelength from said laser cavity via said dichroic mirror, said modelocked fiber laser further comprising a wavelength-division multiplexing (WDM) coupler coupled to said pigtail fiber and said output, for separating the amplified laser energy at the signal wavelength from the laser energy at the pump wavelength and for directing the amplified laser energy at the signal wavelength into said output fiber.
  - 15. The modelocked fiber laser according to claim 14, wherein said pigtail fiber and said WDM coupler are polarization maintaining.
  - 16. The modelocked fiber laser according to claim 15, wherein polarization axes of said pigtail fiber are aligned with the first and second polarization axes of said highly-birefringent fiber gain medium, such that the output of said modelocked laser is obtained along one of said first and second polarization axes.
  - 17. The modelocked fiber laser according to claim 12, wherein said pigtail fiber is coupled to said dichroic mirror via a rotary splice.
  - 18. The modelocked fiber laser according to claim 12, wherein said pigtail fiber is coupled to said dichroic mirror via a glued splice or a fused splice.
  - 19. The modelocked fiber laser according to claim 1, wherein said pump laser is a single-mode laser diode.
  - 20. The modelocked fiber laser according to claim 1, wherein said saturable absorber has a band edge within 100 nm of said signal wavelength.
  - 21. The modelocked fiber laser according to claim 1, wherein said saturable absorber is a semiconductor saturable absorber mirror formed of InGaAsP.
  - 22. The modelocked fiber laser according to claim 1, wherein the second end of said highly-birefringent fiber gain medium is glued to said saturable absorber mirror.
  - 23. The modelocked fiber laser according to claim 1, wherein the second end of said highly-birefringent fiber gain medium is separated from said saturable absorber by a gap.
  - 24. The modelocked fiber laser according to claim 23, wherein the second end of said highly-birefringent fiber gain medium is AR-coated, the modelocked fiber laser further comprising a glass capillary having a first end glued to the AR-coated second end of said highly-birefringent fiber gain medium and a second end glued to said saturable absorber.
  - 25. The modelocked fiber laser according to claim 1, wherein the second end of said highly-birefringent fiber gain medium is attached to said saturable absorber using a lift-off technique.
  - 26. The modelocked fiber laser according to claim 1, wherein said saturable absorber comprises at least one quantum well.
  - 27. The modelocked fiber laser according to claim 1, further comprising an isolator coupled to said pump laser for isolating said pump laser from feedback.
  - 28. The modelocked fiber laser according to claim 1, wherein said output fiber is coupled to said saturable absorber, said saturable absorber comprising a saturable absorber mirror which is partially transmissive at the signal wavelength, to constitute said output for the amplified laser energy.
  - 29. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium is a highly-birefringent double-clad fiber and said pump laser is one of a broad-area diode laser and a diode array.
  - 30. The modelocked fiber laser according to claim 29, further comprising:
    - a double-clad pigtail fiber connecting said pump laser to said reflector, said reflector comprising a dichroic mirror that is at least partially transmissive at the pump wavelength such that the laser energy from said pump laser is transmitted into said laser cavity, said dichroic mirror being partially transmissive at the signal wavelength such that the amplified laser energy is transmitted from said laser cavity to said double-clad pigtail fiber; and
      
      a wavelength-division multiplexing (WDM) coupler coupled to said double-clad pigtail fiber and said output fiber, for separating the amplified laser energy at the signal wavelength from the laser energy at the pump wavelength and for directing the amplified laser energy at the signal wavelength into said output fiber, said WDM coupler operating on a single-mode portion of said double-clad pigtail fiber.
  - 31. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium is coupled to said pump laser via a side-pumping mechanism.
  - 32. The modelocked fiber laser according to claim 1, wherein said saturable absorber comprises an integrated polarizer.
  - 33. The modelocked fiber laser according to claim 32, wherein said integrated polarizer is a wire grid formed on a surface of said saturable absorber, said wire grid being aligned with one of said first and second polarization axes of said highly-birefringent fiber gain medium, such that modelocking is induced along a predetermined one of said first and second polarization axes of said highly-birefringent fiber gain medium.
  - 34. The modelocked fiber laser according to claim 1, wherein a polarization of the laser energy generated by said laser pump is aligned with one of said first and second polarization axes of said highly-birefringent fiber gain medium to produce a differential gain along the first and second polarization axes, which differential gain causes modelocking to occur along a predetermined one of said first and second polarization axes.
  - 35. The modelocked fiber laser according to claim 1, further comprising a polarization-dependent feedback device external to said laser cavity, for generating a polarization-dependent feedback which induces modelocking along a predetermined one of said first and second polarization axes.
  - 36. The modelocked fiber laser according to claim 35, wherein said polarization-dependent feedback device is one of a fiber grating and an external polarizer, in conjunction with a reflecting surface.
  - 37. The modelocked fiber laser according to claim 1, further comprising a piezoelectric coil on which said highly-birefringent fiber gain medium is mounted, said piezoelectric coil being modulated to control an effective length of said laser cavity and to induce modelocking along a predetermined one of said first and second polarization axes of said highly-birefringent fiber gain medium.
  - 38. The modelocked fiber laser according to claim 1, wherein said highly-birefringent fiber gain medium comprises a first optical fiber and a second optical fiber which are spliced together such that polarization axes of said first and second optical fibers are aligned either parallel or anti-parallel to one another.
  - 39. The modelocked fiber laser according to claim 38, wherein said first optical fiber is a double-clad fiber and said second optical fiber is a highly-birefringent, dispersion-compensating fiber.
  - 40. The modelocked fiber laser according to claim 1, wherein the second end of said highly-birefringent fiber gain medium is tapered to increase a mode-field diameter of said highly-birefringent fiber gain medium to thereby increase a damage threshold of said saturable absorber mirror.
  - 41. The modelocked fiber laser according to claim 1, wherein the second end of said highly-birefringent fiber gain medium is separated from said saturable absorber mirror by a distance less than 10 cm.
  - 42. The modelocked fiber laser according to claim 1, further comprising a lens assembly disposed between the second end of said highly-birefringent fiber gain medium and said saturable absorber mirror, for controlling a spot size of the amplified laser energy from said highly-birefringent fiber gain medium on said saturable absorber mirror.
  - 43. The modelocked fiber laser according to claim 1, further comprising an intra-cavity fiber end configured to induce a polarization-dependent loss, for ensuring modelocking along a selected polarization axis.
  - 44. The modelocked fiber laser according to claim 1, further comprising an all-fiber, intra-cavity polarizer.
  - 45. The modelocked fiber laser according to claim 44, wherein said all-fiber, intra-cavity polarizer comprises a polished-down fiber having a metal film deposited thereon.
  - 46. The modelocked fiber laser according to claim 1, wherein said output is coupled to a polarization maintaining fiber pigtail.
  - 47. The modelocked fiber laser according to claim 1, wherein said output is coupled to a fiber pigtail.
  - 48. The modelocked fiber laser according to claim 1, wherein a fiber grating is written into said highly-birefringent fiber gain medium.
  - 49. The modelocked fiber laser according to claim 1, wherein the power of the laser energy generated by said pump laser is varied to induce passive harmonic modelocking and generation of multiple simultaneous pulses in said laser cavity.

50. A method for passively modelocking a fiber laser, comprising the steps of:
- forming a laser cavity from a fiber structure having at least one highly-birefringent fiber gain medium, each said medium having first and second polarization axes, first and second ends of said fiber structure respectively defining first and second ends of the laser cavity;
  
  pumping laser energy at a pump wavelength into the laser cavity;
  
  inducing modelocking in the laser cavity along one of the first and second polarization axes of the highly-birefringent fiber gain medium in the absence of any non-fiber, intra-cavity, polarization-manipulating elements by coupling a reflector to the first end of the laser cavity and by coupling a saturable absorber to the second end of the laser cavity; and
  
  outputting laser energy from the laser cavity at a signal wavelength.
- View Dependent Claims (51, 52, 53, 54, 55, 56, 57, 58, 59)
- - 51. The method according to claim 50, wherein the polarization axis of the highly-birefringent fiber gain medium along which modelocking is induced is indeterminate prior to pumping the laser energy into the laser cavity.
  - 52. The method according to claim 50, further comprising the step of:
    - bending the highly-birefringent fiber gain medium such that a loss differential exists between the first and second polarization axes, which loss differential causes modelocking to occur along a predetermined one of the first and second polarization axes.
  - 53. The method according to claim 52, wherein said bending step includes coiling a portion of the highly-birefringent fiber gain medium with a coiling diameter between approximately 5 mm and 10 cm, and preferably between 12.5 mm and 10 cm.
  - 54. The method according to claim 52, wherein said bending step includes coherently bending the highly-birefringent fiber gain medium such that an orientation of the first and second polarization axes is controlled with respect to a bend of the highly-birefringent fiber gain medium.
  - 55. The method according to claim 50, further comprising the step of:
    - aligning a polarization axis of the laser energy at the pump wavelength with one of the first and second polarization axes of the highly-birefringent fiber gain medium, such that modelocking is induced along a predetermined one of the first and second polarization axes.
  - 56. The method according to claim 50, further comprising the step of:
    - integrating a polarizer into the saturable absorber mirror, the polarizer being aligned with respect to the first and second polarization axes of the highly-birefringent fiber gain medium such that modelocking is induced along a predetermined one of the first and second polarization axes.
  - 57. The method according to claim 50, further comprising the step of:
    - generating, external to the laser cavity, a polarization-dependent feedback which induces modelocking along a predetermined one of the first and second polarization axes of the highly-birefringent fiber gain medium.
  - 58. The method according to claim 50, further comprising the steps of:
    - mounting the highly-birefringent fiber gain medium on a piezoelectric coil; and
      
      modulating the piezoelectric coil to induce modelocking along a predetermined one of the first and second polarization axes of the highly-birefringent fiber gain medium.
  - 59. The method according to claim 50, further comprising the step of:
    - forming an all-fiber polarizer within the laser cavity to induce modelocking along a predetermined one of the first and second polarization axes of the highly-birefringent fiber gain medium.

60. A modelocked fiber laser, comprising:
- a pump laser for generating laser energy at a pump wavelength;
  
  a highly-birefringent fiber gain medium having first and second polarization axes, for amplifying the laser energy at a signal wavelength;
  
  a reflector for reflecting the laser energy through said highly-birefringent fiber gain medium;
  
  a saturable absorber for inducing modelocking of said fiber laser along either one of said first and second polarization axes of said highly-birefringent fiber gain medium in the absence of any non-fiber, intra-cavity, polarization-manipulating elements; and
  
  an output for outputting the laser energy.

61. A modelocked fiber laser, comprising:
- a pump laser for generating laser energy at a pump wavelength;
  
  a highly-birefringent fiber gain medium having first and second polarization axes, for amplifying the laser energy at a signal wavelength;
  
  a reflector for reflecting the laser energy through said highly-birefringent fiber gain medium;
  
  a saturable absorber for inducing modelocking of said fiber laser along either one of said first and second polarization axes of said highly-birefringent fiber gain medium; and
  
  an output for outputting the laser energy.

62. A modelocked fiber laser, comprising:
- a pump laser for generating laser energy at a pump wavelength;
  
  a highly-birefringent double-clad fiber gain medium having first and second polarization axes, for amplifying the laser energy at a signal wavelength;
  
  a side-pumping device for coupling said pump laser to said highly-birefringent double-clad fiber gain medium;
  
  a reflector for reflecting the laser energy through said highly-birefringent fiber gain medium;
  
  a saturable absorber for inducing modelocking of said fiber laser along either one of said first and second polarization axes of said highly-birefringent double-clad fiber gain medium; and
  
  an output for outputting the laser energy.

63. A modelocked fiber laser, comprising:
- a pump laser for generating laser energy at a pump wavelength;
  
  a highly-birefringent fiber gain medium having first and second polarization axes and having first and second ends which respectively define first and second ends of a laser cavity for amplifying the laser energy at a signal wavelength;
  
  a reflector coupled to the first end of said laser cavity, for reflecting the laser energy through said highly-birefringent fiber gain medium;
  
  a saturable absorber for inducing modelocking of said fiber laser along either of said first and second polarization axes of said highly-birefringent fiber gain medium; and
  
  an output for outputting the laser energy amplified within said laser cavity.

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Current Assignee
IMRA America Incorporated (Aisin Corp.)
Original Assignee
IMRA America Incorporated (Aisin Corp.)
Inventors
Harter, Donald J., Fermann, Martin E.
Primary Examiner(s)
Healy, Brian

Application Number

US09/021,863
Time in Patent Office

846 Days
Field of Search

372/11, 372/18, 372/19, 372/20, 372/25, 372/6, 372/43, 372/50, 372/69, 372/70, 372/75, 372/98, 372/101, 372/102, 372/106, 372/105, 385/14, 385/11, 385/37
US Class Current

372/11
CPC Class Codes

H01S 3/067 Fibre lasers

H01S 3/1118 Semiconductor saturable abs...

Integrated passively modelocked fiber lasers and method for constructing the same

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Integrated passively modelocked fiber lasers and method for constructing the same

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