Fiber laser and methods manufacture and use

• US 20070098023A1
• Filed: 10/28/2005
• Published: 05/03/2007
• Est. Priority Date: 10/28/2005
• Status: Abandoned Application

• Current Assignee: Quantronix Incorporated (Schneider Electric SE)
• Original Assignee: Quantronix Incorporated (Schneider Electric SE)
• Inventors: Lu, Wei, Xu, Lin, Sartania, Zaza
• Application Number:
  US11/262,241
• Publication Number:
  US 20070098023A1
• Time in Patent Office: Days
• US Class Current: 372/6
• 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 3/07 consisting of a plurality of parts, e.g. segments H01S3/067 takes precedence
• CPC Class Codes: H01S 3/094011 with bidirectional pumping, i.e. with injection of the pump light from both two ends of the fibre
• CPC Class Codes: H01S 3/106 by controlling devices placed within the cavity H01S3/10076, H01S3/13 take precedence
• CPC Class Codes: H01S 3/1112 Passive mode locking

Abstract

Fiber lasers include a fiber polarization controller to compensate for polarization variation In addition, fiber lasers include dual gain fibers to provide broader bandwidth for ultrashort pulse generation and amplification.

Claims

1. A fiber laser, comprising:

a laser cavity having a first end and a second end, the laser cavity comprising

a first reflector disposed at the first end of the laser cavity,

a second reflector disposed at the second end of the laser cavity to create with the first reflector a resonant oscillator within the laser cavity,

a gain fiber disposed between the first and second reflectors and configured and arranged to amplify a beam of light,

a fiber polarization controller configured and arranged to alter polarization of light in fiber and disposed between the first and second reflectors to modify the polarization of light oscillating within the laser cavity, and

an in-fiber polarizer disposed to receive light from the fiber polarization controller and polarize the received light;

a pump light source to provide a pump beam for the gain fiber; and

an outlet for removing an output beam from the laser cavity.

2. The fiber laser of claim 1, further comprising a mode-locking unit disposed in the cavity to sharpen pulses of light.

3. The fiber laser of claim 1, wherein the fiber polarization controller comprises an optical fiber and a stress inducer, wherein the fiber polarization controller is configured and arranged to produce stress birefringence in the optical fiber to alter polarization of light traveling through the fiber.

4. The fiber laser of claim 1, further comprising a saturable absorber disposed between the two reflectors.

5. The fiber laser of claim 1, wherein the outlet comprises a second fiber polarization controller to modify the polarization of the output beam in an optical fiber.

6. The fiber laser of claim 1, wherein the outlet comprises a second gain fiber to amplify the output beam.

7. The fiber laser of claim 6, wherein the outlet comprises a second pump light source to provide a pump beam to the second gain fiber.

8. The fiber laser of claim 1, wherein the outlet comprises a frequency doubling material disposed to receive the output beam and double a frequency of the output beam.

9. The fiber laser of claim 8, wherein the frequency doubling material is configured and arranged to double the frequency of the output beam at a temperature of no more then 40°

C.

10. The fiber laser of claim 8, wherein the frequency doubling material comprises periodically poled magnesium doped lithium niobate or periodically poled magnesium doped stoichiometric lithium tantalate.

11. The fiber laser of claim 1, wherein the laser cavity is linear.

12. The fiber laser of claim 1, wherein the laser cavity does not contain polarization-maintaining optical fiber.

13. The fiber laser of claim 1, wherein the first reflector is a grating.

14. A fiber laser, comprising:

a laser cavity comprising a gain fiber;

a pump light source coupled to the laser cavity to provide a pump beam to the gain fiber;

an outlet from the laser cavity to provide an output beam; and

a frequency doubling unit to double the frequency of the output beam, the frequency doubling unit comprising a frequency doubling material capable of doubling the frequency of the output beam at a temperature of no greater than 40°

C.

15. The fiber laser of claim 14, wherein the frequency doubling material is selected from periodically poled magnesium doped lithium niobate and periodically poled magnesium doped stoichiometric lithium tantalate.

16. The fiber laser of claim 14, wherein an acceptance bandwidth of the frequency doubling material is at least as broad as a bandwidth of a beam received by the frequency doubling unit.

17. A method for generating laser pulses, the method comprising:

injecting a pump beam into a gain fiber disposed in a laser cavity to generate a laser beam within the cavity;

modifying the polarization of the laser beam in an optical fiber disposed in the cavity using a polarization controller;

directing the laser beam through an in-fiber polarizer after the polarization of the laser beam is modified by the polarization controller; and

coupling a portion of the laser beam out of the laser cavity to form an output beam.

18. The method of claim 17, further comprising sharpening pulses of the laser beam using a saturable absorber.

19. The method of claim 17, further comprising modifying the polarization of the output beam in an optical fiber using a polarization controller.

20. The method of claim 17, further comprising doubling a frequency of the output beam using a frequency doubling material at a temperature of no more than 40°

C.

21. The method of claim 17, further comprising doubling a frequency of the output beam using a frequency doubling material selected from periodically poled magnesium doped lithium niobate and periodically poled magnesium doped stoichiometric lithium tantalate.

22. The method of claim 17, further comprising amplifying the output beam using a second gain fiber and a second pump beam.

23. A fiber laser, comprising:

a laser cavity having a first end and a second end, the laser cavity comprising

a first reflector disposed at the first end of the laser cavity,

a second reflector disposed at the second end of the laser cavity to create with the first reflector a resonant oscillator within the laser cavity,

a first gain fiber disposed between the first and second reflectors, and

a second gain fiber disposed between the first gain fiber and the first reflector, wherein the first and second gain fibers have overlapping gain bandwidths with different peaks;

at least one pump light source to provide a pump beam for the first and second gain fibers; and

an outlet for removing an output beam from the laser cavity.

24. The fiber laser of claim 23, wherein the fiber laser comprises only one pump light source to pump the first and second gain fibers.

25. The fiber laser of claim 23, wherein the fiber laser comprises two pump light sources coupled into the laser cavity on opposite sides of the first and second gain fibers.

26. The fiber laser of claim 23, further comprising a long period grating disposed in the laser cavity to receive output from the first and second gain fibers.

27. The fiber laser of claim 23, wherein the outlet comprises a pair of second gain fibers to amplify the output beam.

28. The fiber laser of claim 23, further comprising a fiber polarization controller configured and arranged to alter polarization of light in fiber and disposed between the first and second reflectors to modify the polarization of light oscillating within the laser cavity, and an in-fiber polarizer disposed to receive light from the fiber polarization controller and polarize the received light.