High energy, ultrashort pulse ring fiber laser having a linear dispersion compensator with chirped Bragg gratings

• US 20080025348A1
• Filed: 07/28/2006
• Published: 01/31/2008
• Est. Priority Date: 07/28/2006
• Status: Abandoned Application

• Current Assignee: Corning Incorporated
• Original Assignee: Corning Incorporated
• Inventors: Kuksenkov, Dmitri Vladislavovich, Li, Shenping
• Application Number:
  US11/495,204
• Publication Number:
  US 20080025348A1
• Time in Patent Office: Days
• US Class Current: 372/6
• CPC Class Codes: H01S 2301/08 Generation of pulses with special temporal shape or frequency spectrum
• CPC Class Codes: H01S 3/06712 Polarising fibre; Polariser
• CPC Class Codes: H01S 3/06725 Fibre characterized by a specific dispersion, e.g. for pulse shaping in soliton lasers or for dispersion compensating [DCF]
• 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 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/1053 Control by pressure or deformation
• CPC Class Codes: H01S 3/1112 Passive mode locking

Abstract

A high energy, ultra short pulse ring fiber laser is provided that includes a passively mode locked, all optical fiber laser formed from a closed loop of optical fiber doped with erbium or other rare earth metal, a pump light source optically coupled to the loop of optical fiber, and a linear dispersion compensator that includes a pair of chirped Bragg gratings with substantially equal but opposite sign dispersion. The difference in dispersion between the pair of chirped Bragg gratings is adjusted so that it is substantially equal and opposite to the dispersion generated in the loop of optical fiber. The linear dispersion compensator includes a tuner which can individually stretch or compress the pair of chirped fiber Bragg gratings such that one of the gratings can be adjusted to cancel out the dispersion of the ring laser cavity, while the other grating is adjusted to eliminate third order dispersion of the cavity.

Claims

1. A high energy, ultrashort pulse fiber laser, comprising:

a passively mode locked, all optical fiber ring laser including a loop of optical fiber doped with a material that provides gain that defines a ring lasing cavity;

a pump light source optically coupled to said loop of optical fiber, and

a linear dispersion compensator including at least one chirped Bragg fiber grating optically coupled to said closed loop of optical fiber.

2. The high energy, ultrashort pulse fiber laser as defined in claim 1, wherein said linear dispersion compensator includes a pair of chirped fiber Bragg gratings with opposite sign dispersion optically coupled to said loop of optical fiber such that a net difference in dispersion between said first and second fiber Bragg gratings is substantially equal and opposite to dispersion generated in said loop of optical fiber.

3. The high energy, ultrashort pulse fiber laser as defined in claim 1, wherein said at least one chirped fiber Bragg grating is optically coupled to said loop of optical fiber by an optical circulator.

4. The high energy, ultrashort pulse fiber laser as defined in claim 1, wherein said pump light source is optically coupled to said loop of optical fiber by a wave division multiplexer.

5. The high energy, ultrashort pulse fiber laser as defined in claim 1, further comprising a polarization controller optically coupled to said loop of optical fiber for passively mode locking the optical fiber ring lasing cavity.

6. The high energy, ultrashort pulse fiber laser as defined in claim 2, wherein said linear dispersion compensator includes a tuner that stretches or compresses one of said pair of chirped fiber Bragg gratings to adjust said net difference in dispersion.

7. The high energy, ultrashort pulse fiber laser as defined in claim 1, wherein the dispersion of the loop of optical fiber is between about −

40 ps/nm-km and −

20 ps/nm-km.

8. The high energy, ultrashort pulse fiber laser as defined in claim 3, wherein said optical circulator is a four-port, polarization maintaining circulator.

9. The high energy, ultrashort pulse fiber laser as defined in claim 1, wherein said lasing dopant in said loop of optical fiber is a rare earth metal.

10. The high energy, ultrashort pulse fiber laser as defined in claim 9, wherein said lasing dopant is erbium.

19. A high energy, ultrashort pulse fiber laser as defined in claim 3, wherein said chirped fiber Bragg gratings are written in polarization maintaining or single polarization optical fiber.

11. A high energy, ultrashort pulse fiber laser, comprising:

a passively mode locked, all optical fiber laser including a loop optical fiber doped with a material that provides gain;

a pump light source optically coupled to said loop of optical fiber, and

a linear dispersion compensator including a pair of chirped Bragg gratings with opposite sign dispersion optically couples to said loop of optical fiber such that a net difference in dispersion between said pair of chirped Bragg gratings is substantially equal and opposite to dispersion generated in said loop of optical fiber.

12. A high energy, ultrashort pulse fiber laser as defined in claim 11, further comprising a polarization controller formed from a plurality of loops in said optical fiber for passively mode locking said all optical fiber laser.

13. A high energy, ultrashort pulse fiber laser as defined in claim 11, wherein said linear dispersion compensation further includes a four-part optical circulator for optically coupling the pair of chirped Bragg gratings to the finger ring lasing cavity.

14. A high energy, ultrashort pulse fiber laser as defined in claim 11, wherein said linear dispersion compensator includes a tuner for varying the bandwidth or the dispersion generated by at least one of the chirped Bragg gratings to adjust one of the net dispersion of the ring laser cavity and a third order dispersion of the cavity.

15. A high energy, ultrashort pulse fiber laser as defined in claim 14, wherein the tuner includes a mechanism for stretching and compression at least one of the chirped Bragg gratings.

16. A high energy, ultrashort pulse fiber laser as defined in claim 11, wherein the loop of optical fiber is a closed loop.

17. A high-energy, ultrashort pulse fiber laser as defined-in claim 11, wherein the doping material is a rare earth metal.

18. A high energy, ultrashort pulse fiber laser as defined in claim 17, wherein the doping material is one for the group consisting of erbium and yttrium.

20. A high energy, ultrashort pulse fiber laser as defined in claim 13, wherein the optical circulator is polarization maintaining.