Method and apparatus for polarization and wavelength insensitive pumping of solid state lasers
View Patent ↗An optical system has a diode pump source, and a gain media made of a material with an anisotropic absorption. The gain media is cut at an angle to produce substantially polarization-independent absorption of a pump beam. An optical coupler is positioned between the diode pump source and the gain media. The optical coupler produces a pump beam that has substantially equal amounts of pump power along any two orthogonal axis that are orthogonal to the pump beam in the gain medium. The wavelength range allowed for the pump source is extended.
1. An optical system that includes a gain media, comprising:
a diode pump source that produces a pump beam;
an optical coupler positioned between the diode pump source and the gain media, the pump beam passing through the optical coupler and
wherein the gain media is cut at a selected angle, and the pump beam, with a selected polarization state, passes through the gain media in a selected direction to provide an increase in a range of wavelengths over which an absorption of the pump beam is constant.
2. The system of claim 1 , wherein the pump beam is substantially unpolarized.
3. The system of claim 1 , wherein the gain media is an ytterbium doped double-tungstate laser crystal.
4. The system of claim 3 , wherein the wavelength of the pump beam is between 931 to 952 nm.
5. The system of claim 1 , wherein the gain media is a thin disk.
6. The system of claim 1 , wherein the pump source is fiber coupled.
7. The system of claim 1 , wherein the coupler includes a polarization beam combiner.
8. The system of claim 1 , wherein the coupler is an imaging coupler.
9. The system of claim 1 , wherein the coupler is a non-imaging coupler.
10. The system of claim 1 , wherein the coupler is a funnel.
11. The system of claim 1 , wherein the pump beam passes through the gain medium multiple times.
12. The system of claim 11 , wherein passage of the pump beam multiple times causes a rotation of a polarization state of the pump beam.
13. The system of claim 11 , further comprising:
a relay optic to re-image the pump beam multiple times into the gain media.
14. The system of claim 1 , further comprising:
a laser resonator, wherein the gain media is positioned in the laser resonator.
15. The laser system of claim 14 , wherein a mode of the resonator is mode-matched to a size of a pumped volume in the gain media.
16. The laser system of claim 14 , further comprising:
wherein the resonator is configured as a regenerative amplifier.
17. The system of claim 1 , further comprising:
wherein the optical system is configured as a single or multi-pass amplifier.
18. The system of claim 1 , wherein the gain media is made of a material selected from, Yb:KGW, Yb:KYW, Yb:S-FAP, Nd:KGW, Nd:KYW, or Nd:YVO 4 , Cr:LiSAF, Cr:Forsterite, and a semiconductor media.
19. A method of broadening an absorption band in a gain media, comprising:
providing an optical system with the gain media made of a material with an anisotropic absorption, the gain media cut at an angle,
selecting a polarization state of a pump beam;
passing the pump beam through the gain media: and
selecting a direction of the pump beam through the gain media to increase a range of wavelengths over which an absorption of the pump beam is constant.
20. The method of claim 19 , wherein a wavelength of the pump beam is at a center of a range of wavelengths over which an absorption of the pump beam is constant.
21. The method of claim 19 , wherein the pump beam is substantially unpolarized.
22. The method of claim 19 , wherein the gain media is an ytterbium doped double-tungstate laser crystal.
23. The method of claim 22 , wherein the wavelength of the pump beam is between 931 to 952 nm.