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

• US 5,880,877 A
• Filed: 01/28/1997
• Issued: 03/09/1999
• 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:
  US08/789,995
• Time in Patent Office: 770 Days
• Field of Search: 359/184, 359/341, 359/346, 359/347, 372/21, 372/22, 372/6
• US Class Current: 359/341.31
• 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 fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source,

wherein pulse compression takes place in said nonlinear fiber amplifier; 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.

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

6. The apparatus according to claim 5, wherein said nonlinear fiber amplifier is doped with one of:

Er³⁺, ErYb⁺, Pr Tm and Ho.

7. The apparatus according to claim 1, wherein the nonlinear fiber amplifier has a numerical aperture (NA) less than 0.15.

8. The apparatus according to claim 1, wherein the nonlinear fiber amplifier has a core area greater than 50 μ

m².

9. The apparatus according to claim 1, wherein said nonlinear fiber amplifier comprises a soliton-Raman compressor (SRC).

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

13. The apparatus according to claim 12, wherein said periodically poled crystal comprises a periodically poled lithium-niobate crystal (PPLN).

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

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

16. The apparatus according to claim 15, further comprising a second pump coupled to said nonlinear fiber amplifier through a second wavelength-division multiplexing coupler, said second pump providing pump light to said nonlinear fiber amplifier.

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

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

19. The apparatus according to claim 1, wherein said nonlinear fiber amplifier is a contradirectionally pumped amplifier and wherein the core diameter and the group-velocity are approximately constant along the amplifier length.

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

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

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

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

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

27. 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 fiber amplifier, and wherein said frequency converter converts energy from a portion of the spectrum of the optical pulses output from said nonlinear fiber amplifier that is greater than the spectral acceptance bandwidth into the spectral acceptance bandwidth.

10. 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.

11. The apparatus according to claim 10, wherein said fiber pulse compressor is a soliton-Raman compressor (SRC).

23. 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 the amplifier fiber is a double-clad fiber, and

wherein pump light and the signal light are launched into a core of the 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.

24. 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.

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

an optical source which generates high power optical pulses;

a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the high power pulses generated by said optical source; and

a frequency converter which receives optical pulses output from said nonlinear fiber 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 of said frequency converter, into the spectral acceptance bandwidth of said frequency converter.

29. The apparatus according to claim 28, wherein said frequency converter is periodically poled.

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

an optical source which generates signal light;

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

a nonlinear fiber compressor which receives optical pulses produced by said amplifier,

wherein the nonlinear fiber compressor has a refractive index distribution which is approximately invariant along the fiber length; and

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

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

means for generating signal light;

optical fiber means for nonlinearly amplifying the signal light;

optical fiber means for pulse compressing the signal light,

wherein the optical fiber means has a refractive index distribution which is approximately invariant along the fiber length; and

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

32. The apparatus according to claim 31, further comprising means for controlling a polarization state of the signal light.

33. The apparatus according to claim 31, further comprising means for pumping pump light into said means for nonlinearly amplifying.

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

generating a signal light;

simultaneously nonlinearly amplifying and pulse compressing the signal light to produce amplified and pulse-compressed optical pulses; and

frequency converting the amplified optical pulses to produce the high-power optical pulses at a different wavelength from the signal light.

35. The method according to claim 34, further comprising the step of:

controlling a polarization state of the signal light.

36. The method according to claim 34, wherein a double-clad fiber performs nonlinear amplification.

37. The method according to claim 36, further comprising the step of launching pump light and the signal light directly into an inner core of the double-clad fiber.

38. 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,

wherein a double-clad fiber, pumped by an optical pumping means performs nonlinear amplification,

further comprising the step of launching pump light and signal light directly into the inner core of said double-clad fiber, and

frequency converting the amplified optical pulses to produce the high-power optical pulses at a different wavelength from the signal light.

39. An apparatus for generating optical pulses, comprising:

a fiber laser source for generating signal light;

a multi-mode fiber amplifier for amplifying the signal light;

means for preferentially launching a fundamental mode of said multi-mode amplifier, said multi-mode amplifier Raman-shifting said fundamental mode; and

frequency conversion means for generating amplified output light at a doubled frequency.

40. 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;

means for preferentially launching a fundamental mode of said multi-mode amplifier, said multi-mode amplifier Raman-shifting said fundamental mode; and

frequency conversion means for generating amplified output light.

41. 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.

42. An apparatus for generating optical pulses, comprising:

an optical source for generating signal light in the form of short optical pulses, and having an emission bandwidth;

a nonlinear amplifier for amplifying the signal light; and

a nonlinear frequency converting element having an acceptance bandwidth which is smaller than said emission bandwidth, and being capable of frequency-converting signal light within a bandwidth larger than said acceptance bandwidth.

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

a fiber laser source for generating signal light in the form of femtosecond regime optical pulses, and having a broad-band emission bandwidth;

an amplifier for amplifying the signal light; and

a nonlinear crystal having an acceptance bandwidth which is smaller than said broad-band emission bandwidth, and being capable of frequency-converting input light within a bandwidth larger than said acceptance bandwidth, for generating narrow-band frequency-converted light from broad-band signal light.

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

a fiber laser source for generating signal light in the form of broad-band femtosecond regime optical pulses;

an amplifier for amplifying the signal light; and

a nonlinear crystal for frequency converting said broad-band signal light into narrow-band frequency-converted light.

45. The apparatus as claimed in claim 44, wherein said nonlinear crystal has an acceptance bandwidth which is smaller than the broad-band emission bandwidth of said signal light, and frequency-converts input light within a bandwidth larger than said acceptance bandwidth.

46. An apparatus for generating optical pulses, comprising:

an optical source for generating signal light in the form of short optical pulses, and having an emission bandwidth;

an amplifier for amplifying the signal light; and

a nonlinear element having a tunable acceptance bandwidth which is smaller than said emission bandwidth, and being capable of frequency-converting said signal light within a bandwidth larger than said acceptance bandwidth.

47. An apparatus as claimed in claim 46, wherein the acceptance bandwidth of said nonlinear element can be tuned within said emission bandwidth without significant decrease in conversion efficiency.

48. An apparatus for generating optical pulses, comprising:

an optical source for generating signal light in the form of short optical pulses, and having an emission bandwidth;

a nonlinear frequency converting element having an acceptance bandwidth which is smaller than said emission bandwidth, and being capable of frequency-converting signal light within a bandwidth larger than said acceptance bandwidth.

49. An apparatus for generating high-power optical pulses for use in two-photon confocal microscopy, 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 pulse compression takes place in said nonlinear fiber amplifier, and said nonlinear fiber amplifier is a polarization maintaining 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.

50. An apparatus for generating high-power optical pulses for use in two-photon confocal microscopy, 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 pulse compression takes place in said nonlinear fiber amplifier, and said nonlinear fiber amplifier is a contradirectionally pumped amplifier, and

wherein the core diameter and the group-velocity are approximately constant along the amplifier 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.

51. An apparatus for generating ultra-short, 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 pulse compression takes place in said nonlinear fiber amplifier; and

a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses in Thz range at an output thereof for use in injection seeding of high-power amplifiers.