Optically pumped semiconductor laser pumped optical parametric oscillator
View Patent ↗An optically pumped semiconductor pumped optical parametric oscillator (OPS-pumped OPO) includes an OPS laser resonator and an OPO resonator A portion the OPS laser resonator axis and the OPO resonator axis are collinear. An optically nonlinear crystal is located in the coaxial portion of the resonators and arranged to frequency divide fundamental radiation generated in the OPS laser resonator into signal and idler radiations. In one arrangement, the OPO laser resonator is also an OPS resonator and is arranged to generate radiation at the wavelength of the signal radiation, with the idler radiation having the difference-frequency wavelength of the signal and fundamental radiations.
1. Optical apparatus, comprising:
an OPS laser resonator including an OPS-structure, the OPS-structure including a mirror-structure and a multilayer semiconductor gain-structure the OPS laser resonator having a resonator-axis folded at least once by a fold-mirror;
an arrangement for energizing the gain-structure of the OPS-structure of the OPS laser resonator thereby causing radiation having a fundamental wavelength to circulate in the OPS laser resonator;
an OPO resonator having an OPO resonator axis folded by a polarizing beamsplitter, a portion of the OPS laser resonator axis and the OPO resonator axis being coaxial; and
an optically nonlinear crystal located in the coaxial portion of the OPS laser and OPO resonators and arranged to frequency divide fundamental wavelength radiation circulating in the OPS laser resonator.
2. The apparatus of claim 1 , wherein the optically nonlinear crystal is arranged for type-II frequency division and the polarizing beamsplitter is arranged to combine the OPS laser resonator axis and the OPO resonator axis into the collinear portion thereof.
3. The apparatus of claim 1 , wherein the optically nonlinear crystal is arranged for type-III frequency division, the OPS laser resonator is folded additionally by the polarizing beamsplitter, the fold-mirror is arranged to combine the OPS laser resonator axis and the OPO resonator axis into the collinear portion thereof, and the polarizing beamsplitter is located in the collinear portion of the resonators.
4. The apparatus of claim 1 , wherein the fold-mirror is a concave mirror.
5. The apparatus of claim 1 , wherein the fundamental radiation is divided into signal radiation having a wavelength longer than the fundamental wavelength and idler radiation having a wavelength longer than the wavelength of the signal radiation, and wherein the apparatus is arranged such that signal radiation circulates in the OPO resonator.
6. The apparatus of claim 5 , wherein the optically nonlinear crystal is one of a KTA crystal and RTA crystal, a KTP crystal, and an LGSE crystal.
7. The apparatus of claim 5 , wherein the OPO resonator also includes an OPS-structure including a mirror-structure and a gain-structure, and an arrangement for energizing the gain-structure, with the gain-structure of the OPS-structure in the OPO resonator being arranged to generate signal wavelength radiation when energized.
8. The apparatus of claim 7 , wherein the optically nonlinear crystal is an LGSE crystal.
9. Optical apparatus, comprising:
an OPS laser resonator including an OPS-structure, the OPS-structure including a mirror-structure and a multilayer semiconductor gain-structure the OPS laser resonator having a resonator-axis folded by a fold-mirror;
an optical pumping arrangement for energizing the gain-structure thereby causing fundamental radiation to circulate in the OPS laser resonator;
an OPO resonator having an OPO resonator axis folded by a polarizing beamsplitter, the polarizing beamsplitter being arranged to combine the OPS laser resonator axis and the OPO resonator axis such that a portion of the OPS laser resonator axis and the OPO resonator axis are coaxial;
an optically nonlinear crystal located in the coaxial portion of the OPS laser and OPO resonators and arranged to frequency divide the fundamental radiation circulating in the OPS laser resonator to provide signal radiation having a wavelength longer than the wavelength of the fundamental radiation, and idler radiation having a wavelength longer than the signal-wavelength radiation; and
wherein signal radiation circulates in the OPO resonator and idler radiation is transmitted by the polarizing beamsplitter and the fold mirror of the OPS laser resonator out of the apparatus.
10. The apparatus of claim 9 , wherein the optically nonlinear crystal is arranged for type-II frequency division, the fundamental and idler radiations are plane-polarized in the same orientation and the signal radiation is plane-polarized in an orientation perpendicular to the polarization-orientation of the fundamental and idler radiations.
11. The apparatus of claim 10 , wherein the polarizing beamsplitter is arranged such that fundamental, signal and idler radiations are non-normally incident thereon and the polarization-orientation of the signal radiation is perpendicular to the plane of incidence of the polarizing beamsplitter.
12. The apparatus of claim 9 , wherein the OPS laser resonator is terminated by the mirror-structure of the OPS-structure and a plane mirror, the OPO resonator is terminated by a concave mirror and the plane mirror, and the fold mirror of the OPS laser resonator is a concave mirror.
13. The apparatus of claim 12 , wherein the concave terminating mirror of the OPO resonator has a radius of curvature and separation from the OPO and OPS resonator plane terminating mirror such that the beam size of the fundamental radiation and the beam size of the signal radiation are about equal.
14. The apparatus of claim 9 , wherein the material of the optically nonlinear crystal is one of a KTA crystal, an RTA crystal, and a KTP crystal.
15. Optical apparatus, comprising:
an OPS laser resonator including an OPS-structure, the OPS-structure including a mirror-structure and a multilayer semiconductor gain-structure the OPS laser resonator having a resonator-axis folded by a fold-mirror and by a polarizing beamsplitter;
an optical pumping arrangement for energizing the gain-structure thereby causing fundamental radiation to circulate in the OPS laser resonator;
an OPO resonator having an OPO resonator axis folded by the polarizing beamsplitter the OPO resonator and OPS laser resonator being arranged such that a portion of the OPS laser resonator axis and the OPO resonator axis are coaxial with the polarizing beamsplitter being located in this coaxial portion of the resonators;
an optically nonlinear crystal located in the coaxial portion of the OPS laser and OPO resonators and arranged to frequency divide the fundamental radiation circulating in the OPS laser resonator to provide signal radiation having a wavelength longer than the wavelength of the fundamental radiation, and idler radiation having a wavelength longer than the signal-wavelength radiation; and
wherein signal radiation circulates in the OPO resonator and idler radiation is transmitted by the polarizing beamsplitter out of the apparatus.
16. The apparatus of claim 15 , wherein the optically nonlinear crystal is arranged for type-III frequency division, the fundamental and signal radiations are plane-polarized in the same orientation and the idler radiation is plane-polarized in an orientation perpendicular to the polarization-orientation of the fundamental and idler radiations.
17. The apparatus of claim 15 , wherein the polarizing beamsplitter is arranged such that fundamental, signal and idler radiations are non-normally incident thereon and the polarization-orientation of the idler radiation is parallel to the plane of incidence of the polarizing beamsplitter.
18. The apparatus of claim 17 , wherein the OPS laser resonator is terminated by the mirror-structure of the OPS-structure and a plane mirror, the OPO resonator is terminated by a concave mirror and the plane mirror, and the fold mirror of the OPS laser resonator is a concave mirror.
19. The apparatus of claim 18 , wherein the concave fold mirror of the OPS resonator is transmissive to signal radiation, the concave terminating mirror of the OPO resonator is positioned such that signal radiation circulates therein through the concave fold mirror of the OPS resonator, and the coaxial portion of the resonators is between the concave fold mirror of the OPS resonator and the plane mirror.
20. The apparatus of claim 15 , wherein the material of the optically nonlinear crystal is one of a KTA crystal, an RTA crystal, and a KTP crystal.
21. Optical apparatus, comprising:
a first OPS laser resonator including a first OPS-structure, the OPS-structure including a mirror-structure and a multilayer semiconductor gain-structure the first OPS laser resonator having a first resonator-axis;
an arrangement for energizing the gain-structure of the first OPS-structure thereby causing radiation having a first wavelength to circulate in the first OPS laser resonator;
a second OPS laser resonator including a second OPS-structure, the second OPS-structure including a mirror-structure and a multilayer semiconductor gain-structure, the second OPS laser resonator having a second resonator-axis and being arranged cooperative with the first OPS laser resonator such that a portion of the first resonator axis is coaxial with the first resonator axis;
an arrangement for energizing the gain-structure of the second OPS-structure thereby causing radiation having a second wavelength to circulate in the second OPS laser resonator, the second wavelength being different from the first wavelength; and
an optically nonlinear crystal located in the coaxial portion of the first and second OPS laser resonators and arranged to generate radiation having the difference-frequency wavelength of the first and second wavelengths.
22. The apparatus of claim 21 , wherein the first OPS laser resonator is terminated by the mirror-structure of the first OPS-structure and a common mirror and the second OPS laser resonator is terminated by the mirror-structure of the second OPS-structure and the common mirror and the coaxial portion of the first and second resonators terminates on the common mirror.
23. The apparatus of claim 22 , wherein the coaxial portion of the first and second OPS laser resonators is folded by a fold mirror reflective for the first and second wavelengths and transmissive for the difference frequency wavelength and the optically nonlinear crystal is located between the fold mirror and the common mirror.
24. The apparatus of claim 23 , wherein the common mirror is highly reflective for the first, second, and third wavelengths whereby the difference frequency radiation is generated by a double-pass of the first and second wavelength radiations through the optically nonlinear crystal and delivered from the apparatus via the fold mirror.
25. The apparatus of claim 21 , wherein the optically nonlinear crystal is an LGSE crystal.