Fiber-or rod-based optical source featuring a large-core, rare-earth-doped photonic-crystal device for generation of narrow-bandwidth high-power pulsed radiation and associated method

• US 7,830,596 B1
• Filed: 05/27/2006
• Issued: 11/09/2010
• Est. Priority Date: 07/29/2005
• Status: Active Grant

• Current Assignee: Lockheed Martin Aculight Corp. (Martin Marietta Corporation)
• Original Assignee: Lockheed Martin Corporation (Martin Marietta Corporation)
• Inventors: Di Teodoro, Fabio, Brooks, Christopher D.
• Primary Examiner(s): BOLDA, ERIC L
• Application Number:
  US11/420,748
• Time in Patent Office: 1,627 Days
• Field of Search: 359/341.1, 385/51, 385/126
• US Class Current: 359/341.1
• CPC Class Codes: C03B 37/10 Non-chemical treatment surface treatment of fibres or filaments made from glass, minerals or slags C03C25/00
• CPC Class Codes: G02B 6/02328 Hollow or gas filled core
• CPC Class Codes: G02B 6/02347 Longitudinal structures arranged to form a regular periodic lattice, e.g. triangular, square, honeycomb unit cell repeated throughout cladding
• CPC Class Codes: G02B 6/02376 Longitudinal variation along fibre axis direction, e.g. tapered holes
• CPC Class Codes: G02B 6/02385 Comprising liquid, e.g. fluid filled holes
• CPC Class Codes: G02B 6/3826 characterised by form or shape
• CPC Class Codes: G02B 6/3853 Lens inside the ferrule lensed connectors G02B6/32
• CPC Class Codes: H01S 3/005 Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping shaping laser beam for working metal or other materials B23K26/06; optical elements, systems or apparatus in general G02B
• CPC Class Codes: H01S 3/0064 Anti-reflection devices, e.g. optical isolaters absorbing layers for marking or protecting purposes in laser working B23K26/50; magneto-optical non-reciprocal devices G02F1/093, G02F1/0955
• CPC Class Codes: H01S 3/0078 Frequency filtering
• CPC Class Codes: H01S 3/06704 Housings; Packages
• CPC Class Codes: H01S 3/06708 Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering optical fibres as passive waveguides G02B6/02
• CPC Class Codes: H01S 3/06729 Peculiar transverse fibre profile
• CPC Class Codes: H01S 3/06741 Photonic crystal fibre, i.e. the fibre having a photonic bandgap
• CPC Class Codes: H01S 3/06745 Tapering of the fibre, core or active region
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/06758 Tandem amplifiers
• CPC Class Codes: H01S 3/094007 Cladding pumping, i.e. pump light propagating in a clad surrounding the active core

Abstract

A method and apparatus use a photonic-crystal fiber having a very large core while maintaining a single transverse mode. In some fiber lasers and amplifiers having large cores problems exist related to energy being generated at multiple-modes (i.e., polygamy), and of mode hopping (i.e., promiscuity) due to limited control of energy levels and fluctuations. The problems of multiple-modes and mode hopping result from the use of large-diameter waveguides, and are addressed by the invention. This is especially true in lasers using large amounts of energy (i.e., lasers in the one-megawatt or more range). By using multiple small waveguides in parallel, large amounts of energy can be passed through a laser, but with better control such that the aforementioned problems can be reduced. An additional advantage is that the polarization of the light can be maintained better than by using a single fiber core.

Claims

1. A method comprising:

providing a first photonic-crystal optical device that includes a first photonic-crystal-defined waveguide having a diameter of at least about 40 microns, and a second photonic-crystal-defined waveguide, wherein the first and second photonic-crystal-defined waveguides each maintain a single transverse mode, and are each surrounded by a cladding to contain pump light so the pump light can enter each waveguide over its length;

generating a pulsed single-frequency narrow-linewidth seed laser signal light;

directing the pulsed seed signal light into the second waveguide of the photonic-crystal optical device;

directing pump light into the second waveguide of the photonic-crystal optical device in a counter-propagating direction relative to the pulsed seed signal light;

amplifying the pulsed seed signal light in the second waveguide while maintaining a single transverse mode to obtain second amplified pulsed signal light;

directing the second amplified pulsed signal light from the second waveguide of the photonic-crystal optical device to the first waveguide of the photonic-crystal optical device;

directing pump light into the first waveguide of the photonic-crystal optical device in a counter-propagating direction relative to the signal light; and

further amplifying the second amplified pulsed signal light in the first waveguide to obtain a first pulsed output beam while maintaining a single transverse mode to a peak power of at least about 300 kW and a spectrally narrow signal bandwidth of less than 50 GHz.

4. The method of claim 1, wherein the first waveguide has a diameter of at least 70 microns.

5. The method of claim 1, wherein the first waveguide has a diameter of at least 100 microns.

6. The method of claim 1, wherein the further amplifying includes outputting the first pulsed output beam with a peak power of at least 1 MW and a spectrally narrow signal bandwidth of less than 20 GHz.

7. The method of claim 1, wherein the further amplifying includes outputting the first pulsed output beam as a near-diffraction-limited pulsed beam having M²<

1.2.

8. The method of claim 1, wherein the further amplifying includes outputting the first pulsed output beam as a linearly polarized pulsed beam.

9. The method of claim 1, wherein the further amplifying includes outputting the first pulsed output beam as a linearly polarized near-diffraction-limited pulsed beam having M²<

1.2.

10. The method of claim 1, wherein the first optical device is a first photonic-crystal fiber and the first waveguide is a first core of the first photonic-crystal fiber, and wherein the further amplifying includes outputting the first pulsed output beam as a linearly polarized near-diffraction-limited pulsed beam having M²<

1.2 and having a degree of polarization of at least 15 dB.

11. The method of claim 1, wherein the first photonic-crystal optical device includes a first photonic-crystal rod having an outer diameter of at least about 1 mm and the first waveguide is a first core of the first photonic-crystal rod and has a diameter of at least 50 microns.

12. The method of claim 1, further comprising:

frequency doubling the first pulsed output beam to obtain frequency-doubled pulses; and

outputting the frequency-doubled pulses at a peak power of at least about 100 kW.

2. A method comprising:

providing a first photonic-crystal optical device that includes a first waveguide having a diameter of at least about 40 microns, wherein the first photonic-crystal optical device also includes a second waveguide that maintains a single transverse mode, wherein the first waveguide and the second waveguide are each surrounded by cladding to contain pump light so the pump light can enter the cores over their lengths;

generating a pulsed narrow-linewidth single-frequency seed laser signal light;

optically coupling the pulsed narrow-linewidth single-frequency seed laser signal light into the second waveguide;

directing pump light into the cladding around the second waveguide in a counter-propagating direction relative to signal light;

amplifying the pulsed signal light in the second waveguide while maintaining a single transverse mode to obtain amplified pulsed signal light; and

directing the amplified pulsed signal light from the second waveguide to the first waveguide; and

further amplifying the amplified pulsed signal light in the first waveguide to obtain a first pulsed output beam while maintaining a single transverse mode to a peak power of at least about 300 kW and a spectrally narrow signal bandwidth of less than 50 GHz.

13. The method of claim 2, wherein the first waveguide has a diameter of at least 70 microns.

14. The method of claim 2, wherein the first waveguide has a diameter of at least 100 microns.

15. The method of claim 2, wherein the further amplifying includes outputting the first pulsed output beam as a pulsed beam having a peak power of at least 4 MW.

16. The method of claim 2, wherein the further amplifying includes outputting the first pulsed output beam as a near-diffraction-limited output beam having M²<

1.2.

17. The method of claim 2, wherein the further amplifying includes outputting the first pulsed output beam as linearly polarized pulses.

18. The method of claim 2, wherein the further amplifying includes outputting the first pulsed output beam as linearly polarized near-diffraction-limited pulses having M²<

1.2.

19. The method of claim 2, wherein the first optical device is a first photonic-crystal fiber and the first waveguide is a first core of the first photonic-crystal fiber, and wherein the further amplifying includes outputting the first pulsed output beam as linearly polarized near-diffraction-limited pulses having M²<

1.2 and having a degree of polarization of at least 15 dB.

20. The method of claim 2, wherein the first photonic-crystal optical device includes a first photonic-crystal rod having an outer diameter of at least about 1 mm and the first waveguide is a first core of the first photonic-crystal rod and has a diameter of at least 50 microns.

21. The method of claim 2, further comprising:

frequency doubling the first pulsed output beam to obtain frequency-doubled pulses; and

outputting the frequency-doubled pulses at a peak power of at least about 100 kW.

3. A method comprising:

providing a first photonic-crystal optical device that includes a first waveguide having a diameter of at least about 40 microns, wherein the first photonic-crystal optical device includes a plurality of segments including a first segment and a second segment, wherein the first segment includes the first waveguide surrounded by a pump cladding and the second segment includes a second waveguide surrounded by a pump cladding;

laser welding the first segment and the second segment to one another side-by-side, wherein the laser welding of the first segment and the second segment to one another occurs before amplifying of pulsed signal light;

generating a pulsed narrow-linewidth single-frequency seed laser signal light;

optically coupling the pulsed seed signal light into the second waveguide;

directing pump light into the cladding around the second waveguide in a counter-propagating direction relative to signal light;

amplifying the pulsed seed signal light in the second waveguide while maintaining a single transverse mode to obtain amplified pulsed signal light; and

directing the amplified pulsed signal light from the second waveguide to the first waveguide; and

further amplifying the amplified pulsed signal light in the first waveguide to obtain a first pulsed output beam while maintaining a single transverse mode to a peak power of at least about 300 kW and a spectrally narrow signal bandwidth of less than 50 GHz.

22. The method of claim 3, wherein the first waveguide has a diameter of at least 70 microns.

23. The method of claim 3, wherein the first waveguide has a diameter of at least 100 microns.

24. The method of claim 3, wherein the further amplifying includes outputting the first pulsed output beam as pulses having a peak power of at least 4 MW.

25. The method of claim 3, wherein the further amplifying includes outputting the first pulsed output beam as a near-diffraction-limited pulses having M²<

1.2.

26. The method of claim 3, wherein the further amplifying includes outputting the first pulsed output beam as linearly polarized pulses.

27. The method of claim 3, wherein the further amplifying includes outputting the first pulsed output beam as linearly polarized near-diffraction-limited output pulses having M²<

1.2.

28. The method of claim 3, wherein the first optical device is a first photonic-crystal fiber and the first waveguide is a first core of the first photonic-crystal fiber, and wherein the further amplifying includes outputting the first pulsed output beam as linearly polarized near-diffraction-limited pulses having M²<

1.2 having a degree of polarization of at least 15 dB.

29. The method of claim 3, wherein the first photonic-crystal optical device includes a first photonic-crystal rod having an outer diameter of at least about 1 mm and the first waveguide is a first core of the first photonic-crystal rod and has a diameter of at least 50 microns.

30. The method of claim 3, further comprising:

frequency doubling the first pulsed output beam to obtain frequency-doubled pulses; and

outputting the frequency-doubled pulses at a peak power of at least about 100 kW.