Anisotropic beam pumping of a Kerr lens modelocked laser
Apparatus and methods for anisotropic pumping of a Kerr lens modelocked laser. Direct diode laser pumping of an ultrafast Kerr lens modelocked laser oscillator is accomplished. Diode lasers generate severely anisotropic beams, meaning the pump beam has a higher-beam-quality dimension and a lower-beam-quality dimension. By spatially overlap of the pump beam higher-beam-quality dimension and the KLM laser mode, KLM operation is accomplished. Multiple laser diode pump beams are combined in counterpropagating and same-side configurations.
1. A direct laser diode pumped, Kerr lens modelocked, laser comprising:
an oscillator cavity including a gain medium;
a diode pump laser that generates an anisotropic pump beam, wherein the pump beam has a higher-beam-quality dimension and a lower-beam-quality dimension, and wherein the pump beam wavelength falls within the absorption band of the gain medium; and
optics for directly coupling the pump beam into the gain medium;
the elements constructed and arranged such that when the laser is modelocked, spatial overlap of the pump beam higher-beam-quality dimension and the KLM laser mode is improved, over spatial overlap of the pump beam higher-beam-quality dimension and the continuous wave mode.
2. The laser of claim 1 wherein the pump beam wavelength is within the full width at half maximum of the absorption curve of the gain medium.
3. The laser of claim 2 wherein the M 2 quality of the lower-beam-quality dimension is at least about three times the M 2 quality of the higher-beam-quality dimension.
4. The laser of claim 1 wherein the pump beam wavelength is below the full width at half maximum of the absorption curve of the gain medium.
5. The laser of claim 1 wherein the pump beam wavelength is above the full width at half maximum of the absorption curve of the gain medium.
6. The laser of claim 1 wherein the gain medium is a Ti:sapphire crystal.
7. The laser of claim 6 wherein the pump beam wavelength is within the full width at half maximum of the absorption curve of the Ti:sapphire crystal.
8. The laser of claim 7 wherein the M 2 quality of the lower-beam-quality dimension is at least about three times the M 2 quality of the higher-beam-quality dimension.
9. The laser of claim 6 wherein the pump beam wavelength is below the full width at half maximum of the absorption curve of the Ti:sapphire crystal.
10. The laser of claim 6 wherein the pump beam wavelength is above the full width at half maximum of the absorption curve of the Ti:sapphire crystal.
11. A Kerr lens modelocked, ultrafast laser comprising:
an oscillator cavity including a gain medium; and
a pump beam generator for generating an anisotropic pump beam, the pump beam having a higher-beam-quality dimension and a lower-beam-quality dimension, the pump beam wavelength falling within the absorption band of the gain medium;
optics for coupling the pump beam into the gain medium;
the elements constructed and arranged such that when the laser is modelocked, spatial overlap of the pump beam higher-beam-quality dimension and the KLM laser mode is improved, over continuous wave mode.
12. The laser of claim 11 wherein the pump beam wavelength is within the full width at half maximum of the absorption curve of the gain medium.
13. The method of inducing stable Kerr lens modelocking in an ultrafast laser comprising the steps of:
(a) generating an anisotropic pump beam, the pump beam having a higher-beam-quality dimension and a lower-beam-quality dimension, wherein the M 2 quality of the lower-beam-quality dimension is at least about three times the M 2 quality of the higher-beam-quality dimension, the pump beam wavelength falling within an absorption band of a gain medium;
(b) coupling the pump beam into a gain medium of the laser;
(c) constructing and arranging the laser elements such that when the laser is modelocked, spatial overlap of the pump beam higher-beam-quality dimension and the KLM laser mode is improved, over continuous wave mode;
(d) Kerr lens modelocking the ultrafast laser; and
(e) outputting ultrafast pulses.
14. The method of claim 13 wherein the step of generating an anisotropic pump beam generates a pump beam having a wavelength within the full width at half maximum of the absorption curve of the gain medium.
15. The method of claim 14 , wherein step (a) generates two anisotropic beams, and wherein step (b) couples both beams into the gain medium.