Apparatus and method for the generation of high-power femtosecond pulses from a fiber amplifier

• US 6,014,249 A
• Filed: 03/08/1999
• Issued: 01/11/2000
• Est. Priority Date: 01/28/1997
• Status: Expired due to Term

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Galvanauskas, Almantas, Harter, Donald J., Fermann, Martin E.
• Primary Examiner(s): Hellner, Mark
• Application Number:
  US09/263,891
• Time in Patent Office: 309 Days
• Field of Search: 359/341, 372/21, 372/22, 372/6
• US Class Current: 359/341.1
• CPC Class Codes: G02F 1/3542 Multipass arrangements, i.e. arrangements to make light pass multiple times through the same element, e.g. using an enhancement cavity
• CPC Class Codes: G02F 1/3548 Quasi phase matching [QPM], e.g. using a periodic domain inverted structure
• CPC Class Codes: G02F 1/37 for second-harmonic generation G02F1/3532 takes precedence
• CPC Class Codes: H01S 2301/085 solitons
• CPC Class Codes: H01S 3/06712 Polarising fibre; Polariser
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/06758 Tandem amplifiers
• CPC Class Codes: H01S 3/1603 rare earth
• CPC Class Codes: H01S 3/2333 Double-pass amplifiers
• CPC Class Codes: H01S 3/302 in an optical fibre

Abstract

An apparatus generates femtosecond pulses from laser amplifiers by nonlinear frequency conversion. The implementation of nonlinear frequency-conversion allows the design of highly nonlinear amplifiers at a signal wavelength (SW), while still preserving a high-quality pulse at an approximately frequency-doubled wavelength (FDW). Nonlinear frequency-conversion also allows for limited wavelength tuning of the FDW. As an example, the output from a nonlinear fiber amplifier is frequency-converted. By controlling the polarization state in the nonlinear fiber amplifier and by operating in the soliton-supporting dispersion regime of the host glass, an efficient nonlinear pulse compression for the SW is obtained. The generated pulse width is optimized by utilizing soliton compression in the presence of the Raman-self-frequency shift in the nonlinear fiber amplifier at the SW. High-power pulses are obtained by employing fiber amplifiers with large core-diameters. The efficiency of the nonlinear fiber amplifier is optimized by using a double clad fiber (i.e., a fiber with a double-step refractive index profile) and by pumping light directly into the inner core of this fiber. Periodically poled LiNbO₃ (PPLN) is used for efficient conversion of the SW to a FDW. The quality of the pulses at the FDW can further be improved by nonlinear frequency conversion of the compressed and Raman-shifted signal pulses at the SW. The use of Raman-shifting further increases the tuning range at the FDW. For applications in confocal microscopy, a special linear fiber amplifier is used.

Claims

1. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

a nonlinear amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source; and

a frequency converter which receives optical pulses output from said nonlinear amplifier, said frequency converter providing the high-power optical pulses at an output thereof.

2. The apparatus according to claim 1, further comprising a polarization controller disposed between said optical source and said nonlinear amplifier, said polarization controller adjusting a polarization state of the signal light received by said nonlinear amplifier.

3. The apparatus according to claim 2, wherein said polarization controller comprises waveplates.

4. The apparatus according to claim 1, wherein said optical source comprises a fiber oscillator.

5. The apparatus according to claim 1, wherein said nonlinear amplifier comprises an amplifier fiber.

6. The apparatus according to claim 5, wherein said amplifier fiber is rare earth doped.

7. The apparatus according to claim 6, wherein said amplifier fiber is doped with one of:

Er³⁺, ErYb⁺, Pr Tm and Ho.

8. The apparatus according to claim 5, wherein the amplifier fiber has a numerical aperture (NA) less than 0.15.

9. The apparatus according to claim 5, wherein the amplifier fiber has a core area greater than 50 μ

m².

10. The apparatus according to claim 5, wherein said amplifier fiber performs pulse compression.

11. The apparatus according to claim 5, wherein said amplifier fiber comprises a soliton-Raman compressor (SRC).

12. The apparatus according to claim 1, further comprising a pulse compressor disposed to compress the optical pulses output from said nonlinear amplifier.

13. The apparatus according to claim 12, wherein said pulse compressor is a soliton-Raman compressor (SRC).

14. The apparatus according to claim 1, wherein said frequency converter comprises a periodically poled crystal.

15. The apparatus according to claim 14, wherein said periodically poled crystal comprises a periodically poled lithium-niobate crystal (PPLN).

16. The apparatus according to claim 1, wherein said nonlinear amplifier is arranged in a double-pass configuration.

17. The apparatus according to claim 16, further comprising one of:

a Faraday rotator mirror, a fiber polarization controller and a λ

/4 waveplate disposed at one end of said nonlinear amplifier.

18. The apparatus according to claim 1, further comprising an isolator disposed between said optical source and said nonlinear amplifier.

19. The apparatus according to claim 1, further comprising a polarization beam splitter disposed at an output of said nonlinear amplifier.

20. The apparatus according to claim 1, wherein said nonlinear amplifier is arranged in a single-pass configuration.

21. The apparatus according to claim 1, further comprising a first pump coupled to said nonlinear amplifier through a first wavelength-division multiplexing coupler, said first pump providing pump light to said nonlinear amplifier.

22. The apparatus according to claim 21, further comprising a second pump coupled to said nonlinear amplifier through a second wavelength-division multiplexing coupler, said second pump providing pump light to said nonlinear amplifier.

23. The apparatus according to claim 1, wherein said amplifier fiber is a polarization maintaining fiber.

24. The apparatus according to claim 1, further comprising a first polarization controller disposed between said optical source and said nonlinear amplifier and a second polarization controller at an output end of said nonlinear amplifier.

25. The apparatus according to claim 1, wherein said nonlinear amplifier comprises a contra-directionally pumped amplifier.

26. The apparatus according to claim 1, wherein said nonlinear amplifier is an over-length amplifier and comprises an undoped fiber at an output end thereof.

27. The apparatus according to claim 1, wherein said nonlinear amplifier comprises a first amplifier fiber having a first doping and a second amplifying fiber having a second doping.

28. The apparatus according to claim 1, wherein said nonlinear amplifier comprises a double-clad fiber pumped with a diode array laser.

29. The apparatus according to claim 1, wherein pump light and the signal light are launched directly into an inner core of the double-clad fiber.

30. The apparatus according to claim 1, wherein said nonlinear amplifier comprises a multi-mode amplifier fiber.

31. The apparatus according to claim 1, wherein said nonlinear amplifier comprises a dispersion compensating fiber.

32. The apparatus according to claim 1, further comprising a dispersion compensating fiber.

33. The apparatus according to claim 1, wherein a spectral acceptance bandwidth of said frequency converter is smaller than an extent of the spectrum of the optical pulses output from said nonlinear amplifier, and wherein said frequency converter converts energy from a portion of the spectrum of the optical pulses output from said nonlinear amplifier that is greater than the spectral acceptance bandwidth into the spectral acceptance bandwidth.

34. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates high power optical pulses; and

a frequency converter which receives optical pulses produced by a nonlinear amplifier and which provides high-power optical pulses at a frequency-converted wavelength, wherein a spectral acceptance bandwidth of said frequency converter is smaller than an extent of the spectrum of the optical pulses from said optical source, and wherein said frequency converter converts energy from a portion of the spectrum of the optical pulses from said optical source that is greater than the spectral acceptance bandwidth into the spectral acceptance bandwidth.

35. The apparatus according to claim 34, wherein said frequency converter is periodically poled.

36. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

an amplifier which receives the signal light generated by said optical source;

a nonlinear compressor which receives optical pulses produced by said nonlinear amplifier; and

a periodically poled frequency converter which receives optical pulses compressed by said nonlinear compressor and which produces the high-power optical pulses at a frequency-converted wavelength.

37. An apparatus for generating high-power optical pulses, comprising:

means for generating signal light;

means for nonlinearly amplifying the signal light; and

means for frequency converting optical pulses produced by said means for nonlinearly amplifying, said means for frequency converting producing the high-power optical pulses at an output thereof.

38. The apparatus according to claim 37, further comprising means for controlling a polarization state of the signal light.

39. The apparatus according to claim 37, means for compressing optical pulses produced by said means for nonlinearly amplifying.

40. The apparatus according to claim 37, further comprising means for reflecting optical pulses through said means for nonlinearly amplifying, thereby forming a double-pass configuration.

41. The apparatus according to claim 37, further comprising means for pumping pump light into said means for nonlinearly amplifying.

42. A method for generating high-power optical pulses, comprising the steps of:

generating a signal light;

nonlinearly amplifying the signal light to produce amplified optical pulses; and

frequency converting the amplified optical pulses to produces the high-power optical pulses.

43. The method according to claim 42, further comprising the step of:

controlling a polarization state of the signal light.

44. The method according to claim 42, further comprising the step of:

compressing the optical pulses.

45. The method according to claim 42, wherein the optical pulses are compressed during the nonlinearly amplifying step.

46. The method according to claim 42, wherein a double-clad fiber performs nonlinear amplification.

47. The method according to claim 46, further comprising the step of launching pump light and the signal light directly into an inner core of the double-clad fiber.

48. The method according to claim 42, further comprising the step of:

reflecting the optical pulses through an amplifier fiber, thereby forming a double-pass configuration.

49. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source;

a fiber pulse compressor disposed to compress the optical pulses output from said nonlinear fiber amplifier;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and

a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.

50. The apparatus according to claim 49, wherein said fiber pulse compressor is a soliton-Raman compressor (SRC).

51. The apparatus according to claim 50, wherein the soliton-Raman compressor generates a Raman pulse with a center wavelength shifted away from the wavelength of the signal pulse generated by the optical source.

52. The apparatus according to claim 49, wherein the soliton-Raman compressor generates a Raman pulse with a center wavelength shifted away from the wavelength of the signal pulse generated by the optical source.

53. The apparatus according to claim 49, 50 or wherein the wavelength-shifted Raman pulse allows for a certain degree of tunability of the Raman pulse.

54. The apparatus according to claim 49, 50, 52, 53 or 51, where the wavelength of the Raman pulse is shifted between 0 and 20 THz.

55. The apparatus according to claim 49, 50, 52, 53 or 51, where the wavelength of the Raman pulse is shifted by more than 20 THz.

56. The apparatus according to claim 49, 50, 52, 53 or 51, where the amount of wavelength shifting is adjustable by the power level launched into said compressor fiber.

57. The apparatus according to claim 49, 50, 52, 53 or 51, where the acceptance bandwidth of the frequency converter is adjusted to be comparable to or smaller than the spectral extent of the Raman pulse, allowing for tunability of the frequency-doubled wavelength output of the apparatus.

58. The apparatus according to claim 52 or 51, where the said fiber compressor is a polarization maintaining fiber.

59. The apparatus according to claim 52 or 51, where both the nonlinear fiber amplifier and the compressor are comprised of polarization maintaining fiber.

60. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source,

wherein said nonlinear amplifier comprises a multi-mode amplifier fiber, and

wherein the signal light is predominantly launched into the fundamental mode of said multi-mode amplifier fiber; and

a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.

61. The apparatus according to claim 60, wherein the nonlinear fiber amplifier comprises a first fiber, which is single-mode, and a compressor fiber, which is multi-mode.

62. The apparatus according to claim 61, wherein the multi-mode compressor fiber is a soliton-Raman compressor and where Raman-shifting takes place in the multi-mode compressor fiber.

63. The apparatus according to claim 61, where the multi-mode compressor fiber is polarization maintaining.

64. An apparatus for generating optical pulses, comprising:

a pulse laser source for generating signal light;

a multi-mode fiber amplifier for amplifying the signal light predominately in a fundamental mode thereof;

a means for Raman-shifting said fundamental mode; and

frequency conversion means for frequency-converting at least a Raman-shifted fundamental mode output of said multi-mode fiber amplifier.

65. The apparatus according to claim 64, wherein the Raman-shifting means provides wavelength-tunability of the Raman-shifted pulse.

66. The apparatus according to claim 64, where the Raman-shifting means produces a pulse with Raman shift between 0 and 20 THz.

67. The apparatus according to claim 64, where the Raman-shifting means produces a pulse with a Raman shift of more than 20 THz.

68. The apparatus according to claim 64, where the amount of Raman-shifting and the resulting wavelength of the Raman-shifted pulse is adjustable by the power level launched into said Raman-shifting means.

69. The apparatus according to claim 64, where the acceptance bandwidth of the frequency converter means is adjusted to be comparable to or smaller than the spectral extent of the Raman-shifted pulse, allowing for tunability of the frequency-doubled wavelength output of the apparatus.

70. The apparatus according to claim 64, where the said Raman-shifting means comprises one of an undoped-single mode fiber, an undoped multi-mode fiber, a polarization maintaining undoped single-mode fiber, and a polarization maintaining undoped multi-mode fiber.

71. The apparatus according to claim 64, where both the multi-mode amplifier and the Raman-shifting means comprise polarization maintaining fibers.

72. The apparatus according to claim 64, where the Raman-shifting means comprises fibers of different length to control the wavelength of the Raman-soliton.

73. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one nonlinear fiber medium, having a nonlinear phase delay, which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said nonlinear fiber medium;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and

a frequency converter which receives optical pulses output from said nonlinear fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

82. The apparatus according to claim 73, 74, 75, 76, 77, 78, 79, 80 or 81, wherein said

pulse compressor is a soliton-Raman compressor (SRC).

83. The apparatus according to claim 82, wherein the soliton-Raman compressor generates a Raman pulse with a center wavelength shifted away from the wavelength of the signal pulse generated by the optical source.

84. The apparatus according to claim 83, wherein the wavelength-shifted Raman pulse allows for a certain degree of tunability of the Raman pulse.

85. The apparatus according to claim 83, where the amount of wavelength shifting is adjustable by the power level launched into said compressor fiber.

86. The apparatus according to claim 73, 74, 75, 78 or 80, wherein said pulse compressor is a soliton-Raman compressor (SRC) which generates a Raman pulse with a center wavelength shifted away from the wavelength of the signal pulse generated by the optical source, and where the acceptance bandwidth of the frequency converter is adjusted to be comparable to or smaller than the spectral extent of the Raman pulse, allowing for tunability of the frequency-doubled wavelength output of the apparatus.

87. The apparatus according to claim 83, where said at least one pulse compressor is a polarization maintaining fiber.

92. The apparatus according to claim 83, where the said Raman-shifting means comprises one of a doped or undoped-single mode fiber, a doped or undoped multi-mode fiber, a polarization maintaining doped or undoped single-mode fiber, and a polarization maintaining doped or undoped multi-mode fiber.

93. The apparatus according to claim 83, where the Raman-shifting means comprises

fibers of different length to control the wavelength of the Raman-soliton.

74. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber medium which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said fiber medium;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and

a frequency converter which receives optical pulses output from said fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

75. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, and which incorporates at least one pulse compressor for compressing the amplified optical pulses;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and

a frequency converter which receives optical pulses output from said nonlinear fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

88. The apparatus according to claim 75, 76, 77, 78, 79, 80 or 81, wherein said at least one amplifier comprises a multi-mode amplifier fiber, and

wherein the signal light is predominantly launched into the fundamental mode of said multi-mode amplifier fiber.

89. The apparatus according to claim 75, 76, 77, 78, 79, 80 or 81, wherein said at least one fiber amplifier comprises a first fiber, which is single-mode, and wherein said at least one compressor is a compressor fiber, which is multi-mode.

90. The apparatus according to claim 89, wherein the multi-mode compressor fiber is a soliton-Raman compressor and where Raman-shifting takes place in the multi-mode compressor fiber.

91. The apparatus according to claim 89, where the multi-mode compressor fiber is polarization maintaining.

76. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, and which incorporates at least one pulse compressor for compressing the amplified optical pulses and including at least one polarization maintaining portion;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length.

77. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one nonlinear fiber medium, having a nonlinear phase delay, which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said nonlinear fiber medium, at least one of said nonlinear fiber medium and said fiber pulse compressor being polarization maintaining;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length.

78. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber amplifier which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said fiber amplifier;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and

a frequency converter which receives optical pulses output from said nonlinear fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

79. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber amplifier which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said fiber amplifier, and being polarization maintaining;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length.

80. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber amplifier which receives the signal light generated by said optical source, including at least one integrated fiber pulse compressor disposed to compress the amplified optical pulses;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and

a frequency converter which receives optical pulses output from said nonlinear fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

81. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber amplifier which receives the signal light generated by said optical source, including at least one integrated polarization maintaining pulse compressor disposed to compress the amplified optical pulses;

wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length.

94. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one nonlinear fiber medium, having a nonlinear phase delay, which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said nonlinear fiber medium; and

a frequency converter which receives optical pulses output from said nonlinear fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

95. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber medium which receives the signal light generated by said optical source; and

at least one fiber pulse compressor disposed to compress the optical pulses output from said fiber medium; and

a frequency converter which receives optical pulses output from said fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

96. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, and which incorporates at least one pulse compressor for compressing the amplified optical pulses; and

a frequency converter which receives optical pulses output from said nonlinear fiber medium, said frequency converter providing the high-power optical pulses at an output thereof.

97. An apparatus for generating high-power optical pulses, comprising:

an optical source which generates signal light;

at least one fiber amplifier which receives the signal light generated by said optical source, including at least one integrated polarization maintaining pulse compressor disposed to compress the amplified optical pulses.