Modular, high energy, widely-tunable ultrafast fiber source

• US 8,031,396 B2
• Filed: 10/29/2009
• Issued: 10/04/2011
• Est. Priority Date: 05/23/2000
• Status: Expired due to Fees

• 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
• Assistant Examiner(s): Diacou; Ari M
• Application Number:
  US12/608,602
• Publication Number:
  US 20100046066A1
• Time in Patent Office: 705 Days
• Field of Search: 359346-348, 359/341.41, 359/341.42, 359/337.4
• US Class Current: 359/341.5
• CPC Class Codes: H01S 3/0057 Temporal shaping, e.g. pulse compression, frequency chirping soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108
• CPC Class Codes: H01S 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/094019 Side pumped fibre, whereby pump light is coupled laterally into the fibre via an optical component like a prism, or a grating, or via V-groove coupling
• CPC Class Codes: H01S 3/094042 of a fibre laser
• CPC Class Codes: H01S 3/109 Frequency multiplication, e.g. harmonic generation
• CPC Class Codes: H01S 3/1112 Passive mode locking
• CPC Class Codes: H01S 3/1115 using intracavity saturable absorbers
• CPC Class Codes: H01S 3/1616 thulium
• CPC Class Codes: H01S 3/1618 ytterbium
• CPC Class Codes: H01S 3/302 in an optical fibre

Abstract

A modular, compact and widely tunable laser system for the efficient generation of high peak and high average power ultrashort pulses. System compactness is ensured by employing efficient fiber amplifiers, directly or indirectly pumped by diode lasers. Dispersive broadening is introduced by dispersive pulse stretching in the presence of self-phase modulation and gain, resulting in the formation of high-power parabolic pulses. In addition, dispersive broadening is also introduced by simple fiber delay lines or chirped fiber gratings. The phase of the pulses in the dispersive delay line is controlled to quartic order by the use of fibers with varying amounts of waveguide dispersion or by controlling the chirp of the fiber gratings. After amplification, the dispersively stretched pulses can be re-compressed to nearly their bandwidth limit by the implementation of another set of dispersive delay lines. A particularly compact implementation of the whole system uses fiber oscillators in conjunction with fiber amplifiers.

Claims

1. An optical pulse source, comprising:

a diode-pumped passively modelocked fiber laser including a saturable absorber and generating pulses in the 1-1.15 μ

m wavelength region;

a Yb;

fiber amplifier for amplifying an output of said fiber laser; and

an output optical fiber optically connected to said passively mode locked fiber laser, and to said Yb;

fiber amplifier, said output optical fiber receiving pulses from said passively mode locked fiber laser and delivering said pulses to said Yb;

fiber amplifier.

2. An optical pulse source according to claim 1, wherein said passively modelocked fiber laser comprises a Yb:

fiber laser.

3. An optical pulse source according to claim 1, wherein said passively modelocked fiber laser comprises a Nd:

fiber laser.

4. The optical pulse source according to claim 1, further comprising:

a length of delivery fiber optically coupled to an output of said Yb;

fiber amplifier.

5. An optical pulse source according to claim 1, further comprising an optical isolator disposed between said modelocked fiber laser and said Yb:

fiber amplifier.

6. An optical pulse source according to claim 1, wherein said passively modelocked fiber laser comprises a soliton laser.

7. An optical pulse source according to claim 1, wherein said passively modelocked fiber laser operates in a negative dispersion regime.

8. An optical pulse source according to claim 1, wherein said passively modelocked fiber laser operates in a positive dispersion regime.

9. An optical pulse source according to claim 1, wherein said Yb:

fiber amplifier comprises a large-gain, non-linear amplifier.

10. An optical pulse source according to claim 1, further comprising a frequency doubler disposed to receive an output of said Yb:

amplifier, said frequency doubler providing frequency doubled pulses at an output of said doubler.

11. The optical pulse source according to claim 1, wherein said Yb:

fiber amplifier is arranged in such a way as to non-linearly amplify pulses received from said passively mode locked fiber laser.

12. An optical pulse source, comprising:

a diode-pumped passively modelocked fiber laser generating pulses in the 1-1.15 μ

m wavelength region, said laser comprising a gain fiber, a saturable absorber disposed near a first end of said fiber laser and operable to initiate modelocking, wherein said passively modelocked laser is arranged such that a pulse bandwidth within said passively modelocked fiber laser is substantially smaller than a gain bandwidth of Yb;

a Yb;

fiber amplifier for non-linear amplification of an output of said fiber laser.

13. The optical pulse source of claim 12, wherein said passively modelocked fiber laser comprises a Bragg grating disposed near a second end of said fiber laser and having a reflection bandwidth substantially smaller than a gain-bandwidth of Yb.

14. The optical pulse source according to claim 12, further comprising an optical filter disposed between said source and said Yb:

amplifier for further limiting the bandwidth of pulses generated by said modelocked fiber laser.

15. The optical pulse source according to claim 12, wherein both said passively modelocked fiber laser and said Yb:

amplifier comprise at least one polarization maintaining fiber.

16. The optical pulse source according to claim 15, wherein said Yb:

fiber amplifier comprises a parabolic pulse amplifier.

17. An optical pulse source according to claim 12, further comprising a frequency doubler disposed to receive an output of said Yb:

amplifier, said frequency doubler providing frequency doubled pulses at an output of said doubler.

18. An optical pulse source comprising:

a diode-pumped passively modelocked fiber laser generating pulses in the 1-1.15 μ

m wavelength region;

a large gain, non-linear Yb;

fiber amplifier for amplifying an output of said fiber laser; and

an optical fiber configured to receive pulses from said non-linear amplifier, wherein said non-linear amplifier and said optical fiber are arranged in such a way that an output of said non-linear amplifier is subjected to large amounts of self-phase modulation and spectral broadening.

19. The optical pulse source of claim 18, wherein said high gain, non-linear amplifier is configured in such a way that an approximately linear chirped output pulse is emitted as an output pulse from said amplifier, said linearly-chirped output pulse being compressible to a pulse width narrower than at least one pulse width generated with said passively modelocked fiber laser.

20. The optical pulse source according to claim 18, wherein a pulse width and spectral bandwidth of a pulse emitted from said passively mode locked fiber laser is small compared to a corresponding pulse width and bandwidth of a pulse emitted from said amplifier.

21. An optical pulse source according to claim 18, where said high gain amplifier gain is at least 10, and a generated pulse from said passively mode locked fiber laser comprises a pulse bandwidth less than the gain bandwidth of Yb.

22. An optical pulse source according to claim 18, further comprising a frequency doubler disposed to receive an output of said Yb:

amplifier, said frequency doubler providing frequency doubled pulses at an output of said doubler.

23. An optical pulse source comprising:

a diode-pumped passively modelocked fiber laser including a saturable absorber and generating femtosecond pulses in the 1-1.15 μ

m wavelength region;

a Yb;

fiber amplifier for amplifying an output of said fiber laser; and

an optical modulator disposed between said passively modelocked fiber laser and said Yb;

amplifier, said modulator being controllable to reduce the repetition rate of pulses emitted from said modelocked fiber laser, to increase the available pulse energy of pulses amplified with said Yb;

amplifier, and to provide for selection of pulses for amplification with said Yb;

amplifier.

24. The optical pulse source according to claim 23, said optical pulse source comprising a plurality of Yb:

fiber amplifiers, wherein said modulator is disposed between said passively mode locked laser and one of said Yb;

fiber amplifiers.

25. The optical pulse source according to claim 23, wherein said source comprises a cascaded arrangement of Yb:

fiber amplifiers and modulators.

26. An optical pulse source according to claim 23, wherein both said passively mode locked fiber laser and said Yb:

amplifier are diode pumped.

27. An optical pulse source comprising,

a seed laser comprising a passively modelocked fiber laser;

a Yb;

fiber amplifier for amplifying pulses generated by said seed laser, said fiber amplifier generating amplified pulses;

an optical fiber configured to receive said amplified pulses, said optical fiber subjecting said received and amplified pulses to large levels of self-phase modulation that broadens the pulse width of said received and amplified pulses.

28. The optical pulse source according to claim 27, wherein said optical fiber comprises holey fiber.

31. The optical pulse source according to claim 27, wherein a phase shift resulting from said large level of self-phase modulation is in the range from π

to as large as 10*π

.

29. A laser system comprising:

a fiber laser seed source generating pulses in the 1-1.15 um wavelength region which have a spectral bandwidth larger than 0.3 nm and a pulse width between 50 fs and 1 ns;

a frequency-shifting fiber which inputs an output of said fiber laser and outputs an anti-Stokes, blue-shifted output.

30. The laser system according to claim 29, wherein said frequency-shifting fiber has negative dispersion.

32. An optical pulse source comprising:

a seed source generating output pulses in the range of 1-1.15 μ

m;

a large gain Yb;

non-linear fiber amplifier having a core diameter in the range from about 1 μ

m to 50 μ

m, said amplifier configured in such a way that the fundamental mode is excited and propagates in said Yb;

amplifier, said Yb;

amplifier generating parabolic amplified pulses.