Multi-stage optical amplifier having photonic-crystal-rod waveguides and non-photonic-crystal optical fiber interconnects and associated method

• US 7,782,527 B1
• Filed: 05/27/2006
• Issued: 08/24/2010
• 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:
  US11/420,749
• Time in Patent Office: 1,550 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. An apparatus comprising:

an optical amplifier having a first photonic-crystal rod (PCR) that has a rare-earth-doped photonic-crystal core with a diameter of at least 40 microns and a cladding having an outer diameter of at least 1 mm;

a master oscillator operable to generate a seed laser signal operatively coupled to the optical amplifier; and

a first optical component having a solid-body fiber that has a signal waveguide directly optically coupled to the core of the first PCR without a free-space gap, wherein the solid-body fiber does not have a photonic-crystal structure in the optical signal path.

2. The apparatus of claim 1, wherein the core of the first PCR maintains a single transverse mode, is capable of operation with a peak power of at least 500 kW and a spectrally narrow signal bandwidth of less than 20 GHz.

3. The apparatus of claim 1, wherein the core of the first PCR outputs linearly polarized pulses having a peak power of at least about 100 kW and a degree of polarization of at least 15 dB (wherein the degree of polarization is a value of ten times the log (base 10) of the ratio of optical power along the polarization axis to the optical power along the orthogonal axis).

4. The apparatus of claim 1, wherein the core of the first PCR has a diameter of at least 70 microns.

5. The apparatus of claim 1, wherein the optical amplifier further includes a second PCR that has a rare-earth-doped photonic-crystal core with a diameter of at least 40 microns and a cladding having an outer diameter of at least 1 mm, and wherein the signal waveguide of the first optical component is directly optically coupled to the core of the second PCR without a free-space gap.

6. The apparatus of claim 5, further comprising a substrate, wherein the first PCR and the second PCR are arranged side by side such that their cores run parallel to one another, wherein the first PCR and the second PCR are laser welded to the substrate along at least a portion of their sides.

7. The apparatus of claim 6, further comprising a pump-block subassembly operatively coupled to the first PCR, wherein the pump-block subassembly directs pump light into the first PCR in a counter-propagating direction relative to signal light, and directs signal light out from the first PCR.

8. The apparatus of claim 6, further comprising a pump-block subassembly operatively coupled between the second PCR and the first PCR, wherein the pump-block subassembly includes a bandpass optical filter and a dichroic mirror/beamsplitter configured to direct pump light into the second PCR in a counter-propagating direction relative to signal light, and to direct signal light from the second PCR to the first PCR through the bandpass optical filter.

9. An apparatus comprising:

an optical amplifier having a first photonic-crystal rod (PCR) that has a rare-earth-doped photonic-crystal core with a diameter of at least 40 microns and a cladding having an outer diameter of at least 1 mm,

non-photonic-crystal means for forming an optical signal path connected to the core of the first PCR without a free-space gap.

10. The apparatus of claim 9, further comprising means for amplifying optical pulses in the first PCR to a peak power of at least 500 kW and a spectrally narrow signal bandwidth of less than 20 GHz.

11. The apparatus of claim 9, further comprising means for amplifying optical pulses in the first PCR to a peak power of at least about 100 kW and a degree of polarization of at least 15 dB (wherein the degree of polarization is a value of ten times the log (base 10) of the ratio of optical power along the polarization axis to the optical power along the orthogonal axis).

12. The apparatus of claim 9, wherein the provided optical amplifier further includes a second PCR that has a rare-earth-doped photonic-crystal core with a diameter of at least 40 microns and a cladding having an outer diameter of at least 1 mm, wherein the non-photonic-crystal means is also connected to the core of the second PCR without a free-space gap.

13. A method comprising:

providing an optical amplifier having a first photonic-crystal rod (PCR) that has a rare-earth-doped photonic-crystal core with a diameter of at least 40 microns and a cladding having an outer diameter of at least 1 mm,

providing a master oscillator;

providing a solid-body fiber that has a signal waveguide, wherein the solid-body fiber does not have a photonic-crystal structure in the optical signal path;

generating a seed laser signal with the master oscillator;

optically coupling the seed laser signal to the optical amplifier; and

directly optically coupling the signal waveguide of the solid-body fiber to the core of the first PCR without a free-space gap.

14. The method of claim 13, further comprising amplifying optical pulses in the first PCR to a peak power of at least 500 kW and a spectrally narrow signal bandwidth of less than 20 GHz.

15. The method of claim 13, further comprising amplifying optical pulses in the first PCR to a peak power of at least about 100 kW and a degree of polarization of at least 15 dB (wherein the degree of polarization is a value of ten times the log (base 10) of the ratio of optical power along the polarization axis to the optical power along the orthogonal axis).

16. The method of claim 13, wherein the core of the first PCR has a diameter of at least 70 microns.

17. The method of claim 13, wherein the provided optical amplifier further includes a second PCR that has a rare-earth-doped photonic-crystal core with a diameter of at least 40 microns and a cladding having an outer diameter of at least 1 mm, the method further comprising directly optically coupling the signal waveguide of the solid-body fiber to the core of the second PCR without a free-space gap.

18. The method of claim 13, further comprising:

providing a substrate;

arranging the first PCR and the second PCR side by side such that their cores run parallel to one another; and

laser welding the first PCR and the second PCR to the substrate along at least a portion of their sides wherein the laser welding occurs before the generating of the seed laser signal.

19. The method of claim 18, further comprising:

providing a pump-block subassembly;

directing pump light with the pump-block subassembly into the first PCR in a counter-propagating direction relative to signal light; and

directing signal light out from the first PCR.

20. The method of claim 18, further comprising:

providing a pump-block subassembly operatively coupled between the second PCR and the first PCR, wherein the pump-block subassembly includes a bandpass optical filter and a dichroic mirror/beamsplitter;

optically coupling and bandpass filtering signal light from the second PCR into the first PCR using a dichroic mirror/beamsplitter and a filter; and

directing pump light into the second PCR in a counter-propagating direction relative to signal light using dichroic mirror/beamsplitter.