Externally frequency-converted CW hybrid MOPA
View Patent ↗A hybrid CW MOPA includes an OPS-laser resonator delivering radiation in a plurality of longitudinal lasing-modes or wavelengths. The multiple longitudinal mode output is amplified in a fiber-amplifier. Amplified lasing-modes from the fiber-amplifier are frequency-converted by an optically nonlinear crystal in a ring-resonator having the same length as the laser resonator, such that the ring-resonator is resonant for all of the amplified lasing-modes.
1. Laser apparatus, comprising:
an OPS-laser resonator configured to deliver continuous-wave (CW) radiation in a plurality of different longitudinal lasing-wavelengths, the OPS-laser resonator having an optical length determining a wavelength-spacing of the longitudinal lasing-wavelengths;
a fiber-amplifier having a gain-fiber arranged to amplify the lasing-wavelengths of the OPS laser;
a frequency-converter arranged to receive the amplified lasing-wavelengths, the frequency-converter including an optically nonlinear crystal arranged in an enhancement-resonator for converting the plurality of lasing-wavelengths to a corresponding plurality of frequency-converted wavelengths, the enhancement-resonator having an optical length equal to or an integer multiple of the length of the OPS-laser resonator such that the enhancement-resonator provides a plurality of resonance peak-wavelengths having the same wavelength-spacing as the lasing-wavelengths; and
wherein the optical length of the enhancement-resonator is actively adjusted such that the resonance-peak wavelengths thereof having the same wavelength-spacing as the lasing wavelengths are adjusted to be equal to those lasing wavelengths.
2. The apparatus of claim 1 , wherein the gain-fiber has a gain-bandwidth and has a power-handling limit for any one lasing wavelength determined by stimulated Brillouin scattering (SBS) in the fiber, the SBS having a characteristic bandwidth, the wavelength-spacing of the lasing-wavelengths being greater than the SBS-bandwidth.
3. The apparatus of claim 2 , wherein there is a spectrally selective device within the resonator for limiting the lasing wavelengths to within a predetermined wavelength range less than or equal to about the gain-bandwidth of the gain-fiber.
4. The apparatus of claim 3 , wherein the spectrally-selective device is a birefringent filter.
5. The apparatus of claim 3 , wherein the optically nonlinear crystal has an acceptance-bandwidth for conversion and the predetermined wavelength range of the lasing wavelengths is within the acceptance bandwidth of the optically nonlinear crystal.
6. The apparatus of claim 1 , wherein the optically nonlinear crystal is arranged to frequency-double the lasing-wavelengths to provide frequency-converted wavelengths which are one-half the wavelength of corresponding lasing-wavelengths.
7. The apparatus of claim 1 , wherein the optical length of the enhancement-resonator is twice that of the laser resonator and every other resonance-peak wavelength is equal to a corresponding lasing-wavelength.
8. The apparatus of claim 1 , wherein the enhancement resonator is a ring-resonator.
9. The apparatus of claim 1 wherein the gain-fiber is an ytterbium-doped gain fiber.
10. Laser apparatus, comprising:
an OPS-laser resonator configured to deliver continuous-wave (CW) radiation in a plurality of longitudinal lasing-wavelengths, with all lasing-wavelengths within a predetermined wavelength range, the OPS-laser resonator having an optical length determining a wavelength-spacing of the longitudinal lasing-wavelengths;
a fiber-amplifier having a gain-fiber arranged to amplify the lasing-wavelengths of the OPS laser, the gain-fiber having a gain-bandwidth and a power-handling limit for any one lasing wavelength determined by stimulated Brillouin scattering (SBS) in the fiber, the SBS having a characteristic bandwidth, the wavelength range of the plurality of lasing-wavelengths being within the gain-bandwidth of the gain-fiber and the wavelength-spacing of the lasing-wavelengths being greater than the SBS-bandwidth;
a frequency-converter arranged to receive the amplified lasing-wavelengths, the frequency-converter including an optically nonlinear crystal arranged in an enhancement-resonator for converting the plurality of lasing-wavelengths to a corresponding plurality of frequency-converted wavelengths, the enhancement-resonator having an optical length equal to or an integer multiple of the length of the OPS-laser resonator such that the enhancement-resonator provides a plurality of resonance peak-wavelengths having the same wavelength-spacing as the lasing-wavelengths; and
wherein the optical length of the enhancement-resonator is actively adjusted such that the resonance-peak wavelengths thereof having the same wavelength-spacing as the lasing wavelengths are adjusted to be equal to those lasing wavelengths.
11. The apparatus of claim 10 , wherein the optically nonlinear crystal is arranged to frequency-double the lasing-wavelengths to provide frequency-converted wavelengths which are one-half the wavelength of corresponding lasing-wavelengths.
12. The apparatus of claim 10 , wherein the optical length of the enhancement-resonator is twice that of the laser resonator and every other resonance-peak wavelength is equal to a corresponding lasing-wavelength.
13. The apparatus of claim 10 , wherein the enhancement resonator is a ring-resonator.
14. The apparatus of claim 10 wherein the gain-fiber is an ytterbium-doped gain fiber.
15. The apparatus of claim 10 wherein any one of the laser-resonator and the enhancement-resonator includes a dispersion adjusting element arranged such the laser-resonator and the enhancement resonator have about the same total dispersion.
16. The apparatus of claim 15 wherein the dispersion-adjusting element is a refractive element.
17. The apparatus of claim 15 , wherein the dispersion-adjusting element is a reflective element.