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