Mode-locked fiber laser with improved life-time of saturable absorber

• US 9,048,627 B2
• Filed: 12/18/2008
• Issued: 06/02/2015
• Est. Priority Date: 12/18/2007
• Status: Active Grant

• Current Assignee: NKT Photonics A/S (NKT A/S)
• Original Assignee: NKT Photonics A/S (NKT A/S)
• Inventors: Andersen, Thomas Vestergaard, Laegsgaard, Jesper, Leick, Lasse
• Primary Examiner(s): Maldonado, Julio J
• Assistant Examiner(s): King, Joshua
• Application Number:
  US12/808,327
• Publication Number:
  US 20100296529A1
• Time in Patent Office: 2,357 Days
• Field of Search: 372/6, 372/18, 372/29.021, 372/33, 372/99, 372/102
• US Class Current: 1/1
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/08009 using a diffraction grating
• 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

Abstract

A mode locked fiber laser system is arranged to have a lasing bandwidth and having a linear cavity, the cavity including a gain medium, a saturable absorber having a saturation power, and a filter having a spectral response, wherein the mode locked fiber laser system is arranged so that substantial CW mode locked operation is obtainable with less than 3 times the saturation fluence impinging on the saturable absorber.

Claims

1. A mode locked fiber laser system arranged to have an output having a lasing bandwidth and having a linear cavity, said cavity comprising:

a fiber gain medium,

a saturable absorber having a saturation fluence, and

a substantially uniform Bragg grating filter having a spectral response and a bandwidth of less than 3 nm, and

wherein said mode locked fiber laser system is arranged so that substantial CW mode locked operation is obtainable when less than 3 times the saturation fluence is impinging on the saturable absorber, and

the spectral response of the filter is arranged to dampen a spectral broadening relative to the lasing bandwidth;

said system further comprises an output coupler arranged between said substantially uniform Bragg grating filter and said saturable absorber.

2. The mode locked laser system of claim 1, wherein said broadening is at least partially a result of non-linear effects caused by an increase in optical power, such as self phase modulation in an optical fiber comprised by the cavity.

3. The mode locked laser system of claim 1, wherein said Bragg grating filter has a bandwidth of less than 1 nm.

4. The mode locked laser system of claim 1, wherein said Bragg grating filter has a main transmission dip of the spectral response having a depth of more than or equal to 3 dB.

5. The mode locked laser system of claim 1, wherein the spectral response of the Bragg grating filter comprises a substantially flat top extending more than or equal to 30% of the lasing bandwidth.

6. The mode locked laser system of claim 1, wherein the spectral response of the Bram crating filter comprises at least one slope towards lower reflectivity of more than 70% per nm.

7. The mode locked laser system of claim 1, wherein said Bragg grating filter is a fiber Bragg grating filter.

8. The mode locked laser system of claim 1, wherein said Bragg grating filter is shorter than or equal to 10 mm.

9. The mode locked laser system of claim 1, wherein said laser system comprises an optical fibre with low non-linearity.

10. The mode locked laser system of claim 1, wherein said cavity is substantially polarization maintaining.

11. The mode locked laser system of claim 1, having a pulsed output wherein said pulse has a (FWHM) time span of approximately more than 1 ps.

12. The mode locked laser system of claim 1, having an output path, said output path comprising an optical output filter.

13. The mode locked laser system of claim 12, having an output pulse shape having a main peak and an output spectral distribution wherein said optical output filter is arranged to reduce distortion of the output spectral distribution relative to an ideal output spectral distribution.

14. The mode locked laser system of claim 12, wherein said optical output Bragg grating filter is arranged to reduce spikes in the output spectral distribution, caused by said spectral response of the filter.

15. The mode locked laser system of claim 1, wherein said saturable absorber has a saturable absorption of at least 5%.

16. The mode locked laser system of claim 1, wherein said saturable absorber has a saturable absorption of at least 10%.

17. A mode locked fiber laser system arranged to have an output having a lasing bandwidth and a pulse peak power, said system having a linear cavity with a non-linear property, said cavity comprising:

a fiber gain medium,

a saturable absorber, and

a substantially uniform Bragg grating filter having a spectral response and a bandwidth of less than 3 nm,

wherein the spectral response of said filter is arranged to reduce spectral components outside said lasing bandwidth arising from self-phase modulation caused by said non-linear property and an increase in pulse peak power;

said system further comprises an output coupler arranged between said substantially uniform Bragg grating filter and said saturable absorber.

18. A mode locked fiber laser system arranged to have an output having a lasing bandwidth and a pulse power in CW mode-locked operation, said laser having a linear cavity, said cavity comprising:

a fiber gain medium,

a saturable absorber having a saturation fluence, and

a substantially uniform Bragg filter having a spectral response and a bandwidth,

wherein said filter is arranged to exhibit an increased loss outside the lasing bandwidth of less than 3 nm so that a spectral broadening relative to said lasing bandwidth due to an increase in optical pulse power is sufficiently penalized to stabilize the laser in CW mode-locking operation;

said system further comprises an output coupler arranged between said substantially uniform Bragg grating filter and said saturable absorber.

19. The mode locked laser system of claim 18, wherein said loss is arranged so that if pulse energy increases, the increase in spectral broadening leads to a corresponding loss at the Bragg grating filter which then compensate the increase in reflectivity of the saturable absorber.

20. The mode locked laser system of claim 18 wherein said Bram grating filter is arranged such that substantial CW mode locked operation is obtainable with less than 3 times the saturation fluence impinging on the saturable absorber.

21. The mode locked laser system of claim 18 wherein said Bragg grating filter have a bandwidth of less than 1 nm.

22. The mode locked laser system of claim 18 wherein said Bragg grating filter has a main transmission dip of the spectral response having a depth of more than or equal to 3 dB.

23. The mode locked laser system of claim 18 wherein said Bragg grating filter is a fiber Bragg grating filter.

24. The mode locked laser system of claim 18 wherein said Bragg grating filter is shorter than or equal to 10 mm.

25. The mode locked laser system of claim 18 wherein said laser system comprises an optical fiber with low non-linearity.

26. The mode locked laser system of claim 18 wherein said cavity is substantially polarization maintaining.

27. The mode locked laser system of claim 18 having a pulsed output wherein said pulse has a (FWHM) time span of more than 1 ps.

28. The mode locked laser system of claim 18 further having an output path, said output path comprising an optical output filter.

29. The mode locked laser system of claim 18 wherein the saturable absorber is a semiconductor saturable absorber.

30. The mode locked laser system of claim 18 wherein the saturable absorber is a semiconductor absorbable mirror.

31. The mode locked laser system of claim 18, wherein said saturable absorber has a saturable absorption of at least 5%.

32. The mode locked laser system of claim 18, wherein said saturable absorber has a saturable absorption of at least 10%.