Method and apparatus for generating ultrashort pulses with adjustable repetition rates from passively modelocked fiber lasers

• US 5,701,319 A
• Filed: 10/20/1995
• Issued: 12/23/1997
• Est. Priority Date: 10/20/1995
• Status: Expired due to Term

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Fermann, Martin E.
• Primary Examiner(s): Bovernick, Rodney B.
• Assistant Examiner(s): Wise, Robert E.
• Application Number:
  US08/546,062
• Time in Patent Office: 795 Days
• Field of Search: 372/6, 372/11, 372/18, 372/25, 372/30
• US Class Current: 372/18
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/06712 Polarising fibre; Polariser
• CPC Class Codes: H01S 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/094007 Cladding pumping, i.e. pump light propagating in a clad surrounding the active core
• CPC Class Codes: H01S 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
• CPC Class Codes: H01S 3/1118 Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based
• CPC Class Codes: H01S 3/1121 Harmonically mode locking lasers, e.g. modulation frequency equals multiple integers or a fraction of the resonator roundtrip time

Abstract

The generation of ultrashort pulses with adjustable repetition rates from passively modelocked fiber lasers is demonstrated. By inserting semiconductor saturable absorbers with life-times of the order of 10 nsec into fiber lasers with cavity round-trip times of the order of 100 nsec, passive harmonic modelocking is obtained, leading to the stable generation of pulses at integer multiples of the fundamental cavity frequency. For polarization states that allow for optical limiting of the lasers, pulses are obtained in a frequency range between 20 and 500 MHz., where different repetition rates can be simply selected by changing the pump power level to the cavity. The pulse jitter within one cavity round-trip time is measured to be between 300 psec and 50 psec, where side bands in the frequency domain may be suppressed by up to 70 dB. The saturable absorber acts to both stabilize the cavity repetition rate and to initiate passive modelocking, where nonlinear-polarization evolution is used to sustain modelocking and to suppress amplitude fluctuations of the pulses by providing for optical limiting. Practical embodiments can be obtained by employing environmentally stable cavity designs in polarization preserving single-clad and double clad fibers, where the latter fiber designs allow the pumping of the fiber lasers with broad area-diode array lasers.

Claims

1. A passively modelocked laser comprising:

means for optical pumping of the modelocked laser;

an optical cavity for adjusting the energy of said laser;

means for initiating and sustaining the production of short optical pulses in said cavity;

an optical fiber gain medium for transmitting said optical pulses, said optical pulses having a repetition rate of integer multiples of the fundamental cavity frequency;

means for outputting laser energy from said cavity;

means for maximizing the separation of said pulses inside the cavity, including at least one semiconductor saturable absorber with a carrier life time shorter than the fundamental cavity round-trip time and longer than one hundredth of the cavity round-trip time; and

means for providing optical limiting in the cavity to minimize pulse amplitude fluctuations.

2. The modelocked laser according to claim 1, where short pulses are sustained by a fast Kerr-nonlinearity.

3. The modelocked laser according to claim 2, wherein at least one of said saturable absorbers is butted to one end of said cavity, further comprising a partially reflective saturable absorber for output coupling.

4. The modelocked laser according to claim 2, further comprising a partially reflective saturable absorber for output coupling.

5. The modelocked laser according to claim 1, where optical limiting is induced by a fast Kerr-nonlinearity.

6. The modelocked laser according to claim 1, further comprising means for compensating linear phase drifts of said gain medium.

7. The modelocked laser according to claim 6, wherein said gain medium has a birefringence >

1×

10^-7 to stabilize nonlinear pulse shaping by nonlinear polarization evolution.

8. The modelocked laser according to claim 7, further comprising a quarter and a half-wave plate to control the linear phase delay between two polarization eigenmodes of the fiber.

9. The modelocked laser according to claim 8, further comprising a polarizer, at least one cavity mirror, and a second quarter-wave plate located between said polarizer and the cavity mirror closest to the polarizer, for adjustable output coupling.

10. The modelocked laser according to claim 7, further comprising a polarizer, at least one cavity mirror, and a second quarter-wave plate located between said polarizer and the cavity mirror closest to the polarizer, for adjustable output coupling.

11. The modelocked laser according to claim 6, further comprising:

a polarizer located at one end of said cavity;

a double-clad fiber attached to said optical fiber;

wherein said means for reflecting comprises a cavity end mirror located at a second end of said cavity; and

wherein said means for compensating comprises;

a first Faraday rotator located in front of said cavity end mirror; and

a second Faraday rotator.

12. The modelocked laser according to claim 11, further comprising a quarter and a half-wave plate to control the linear phase delay between the two polarization eigenmodes of the fiber.

13. The modelocked laser according to claim 12, further comprising at least one cavity mirror, and a second quarter-wave plate located between said polarizer and the cavity mirror closest to the polarizer, for adjustable output coupling.

14. The modelocked laser according to claim 13, wherein one of said Faraday rotators is combined with a cavity mirror to constitute a Faraday rotator mirror.

15. The modelocked laser according to claim 13, wherein part of said optical fiber has a birefringence >

1e-7 and another part of said optical fiber has a birefringence <

1e-7, and the lower birefringence optical fiber is located in front of said cavity end mirror.

16. The modelocked laser according to claim 12, wherein part of said optical fiber has a birefringence >

1e-7 and another part of said optical fiber has a birefringence <

1e-7, and the lower birefringence optical fiber is located in front of said cavity end mirror.

17. The modelocked laser according to claim 11, wherein one of said Faraday rotators is combined with a cavity mirror to constitute a Faraday rotator mirror.

18. The modelocked laser according to claim 11, wherein part of said optical fiber has a birefringence >

1e-7 and another part of said optical fiber has a birefringence <

1e-7, and the lower birefringence optical fiber is located in front of said cavity end mirror.

19. A modelocked laser according to claim 11, wherein at least on of said saturable absorbers is located at a distance L away from one of the two cavity mirrors, to create a harmonically partitioned cavity.

20. The modelocked laser according to claim 6, wherein at least one of said saturable absorbers is butted to one end of said cavity.

21. The modelocked laser according to claim 6, further comprising a partially reflective saturable absorber for output coupling.

22. The modelocked laser according to claim 6, further comprising a quarter and a half-wave plate to control the linear phase delay between two polarization eigenmodes of the fiber.

23. The modelocked laser according to claim 22, further comprising a polarizer, at least one cavity mirror, and a second quarter-wave plate located between said polarizer and the cavity mirror closest to the polarizer, for adjustable output coupling.

24. The modelocked laser according to claim 1, further comprising means for controlling the dispersion in said cavity, consisting of one of dispersion compensating fiber and chirped fiber Bragg gratings.

25. The modelocked laser according to claim 24, where said chirped fiber Bragg grating is written directly into said gain medium and said gain medium is pumped through said chirped fiber Bragg grating.

26. The modelocked laser according to claim 24, wherein at least one of said saturable absorbers is butted to one end of said cavity.

27. The modelocked laser according to claim 24, further comprising a partially reflective saturable absorber for output coupling.

28. The modelocked laser according to claim 1, wherein said gain medium is a glass-fiber doped with a rare-earth material.

29. The modelocked laser according to claim 1, wherein said gain medium comprises a glass-fiber doped with a rare-earth material and a double cladding, and is pumped by a diode array.

30. The modelocked laser according to claim 1, wherein at least one of said saturable absorbers is butted to one end of said cavity.

31. The modelocked laser according to claim 1, wherein a fiber coupler is used for output coupling.

32. The modelocked laser according to claim 1, further comprising a partially reflective saturable absorber for output coupling.

33. The modelocked laser according to claim 1, where said fiber has a birefringence <

5×

10^-7.

34. The modelocked laser according to claim 1, wherein said optical fiber is arranged to form a ring cavity.

35. The modelocked laser according to claim 1, wherein said cavity comprises a fiber loop.

36. The modelocked laser according to claim 1, wherein said cavity comprises an optical loop.

37. The modelocked laser according to claim 36, further comprising:

one of a single mode and a double-clad fiber gain medium;

a Faraday rotator mirror having a Faraday rotator and a mirror, for compensating for linear phase drifts in said double-clad fiber and said optical fiber;

a polarizer; and

a half-wave plate cooperating with said polarizer to compensate for any polarization rotation induced by said Faraday rotator mirror.

38. A modelocked laser according to claim 1, further comprising wavelength tuning elements including at least one of etalons, optical filters, birefringent tuning plates and bulk gratings.

39. A modelocked laser according to claim 1, wherein one of said saturable absorbers is located at a round-trip distance L away from a cavity mirror, and the rest of said cavity has a round-trip length nL (n=integer), such that a harmonically partitioned Fabry-Perot cavity is obtained.

40. The modelocked laser according to claim 1, wherein said means for pumping comprises a semiconductor diode laser.

41. The modelocked laser according to claim 40, wherein said semiconductor diode laser is one of a single mode diode laser and a diode array laser.

42. The modelocked laser according to claim 1, wherein said fiber has a birefringence >

1×

10^-7.