Solid-state laser system
A method of operating a q-switch RE,XAB laser includes: providing a pump bias current to a pump source, the pump source directed to an RE:XAB gain medium, the RE:XAB gain medium within a resonator cavity, where X is selected from Ca, Lu, Yb, Nd, Sm, Eu, Gd, Ga, Tb, Dy, Ho, Er, and where RE is selected from Lu, Y, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Pr, Tm, Cr, Ho, with a bias current level below a lasing threshold of the RE:XAB gain medium; providing a pump pulse to the gain medium, the pump pulse of the lasing threshold of the RE:XAB gain medium, the pump pulse causing the RE:XAB gain medium to emit a laser pulse; and reducing the pump bias current to at least below the gain medium lasing threshold, the combination of the pump bias, the pump pulse, and the pump reduction having a current profile.
1. A method of operating a q-switch RE,XAB laser, the steps comprising:
providing a pump bias current to a pump source, the pump source directed to an RE:XAB gain medium, the RE:XAB gain medium within a resonator cavity, where X is selected from Ca, Lu, Yb, Nd, Sm, Eu, Gd, Ga, Tb, Dy, Ho, Er, and where RE is selected from Lu, Y, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Pr, Tm, Cr, Ho, with a bias current level below a lasing threshold of the RE:XAB gain medium;
providing a pump pulse to the gain medium, the pump pulse of the lasing threshold of the RE:XAB gain medium, the pump pulse causing the RE:XAB gain medium to emit a laser pulse; and
reducing the pump bias current to at least below the gain medium lasing threshold, the combination of the pump bias, the pump pulse, and the pump reduction having a current profile.
2. The method of claim 1 , wherein the pump source has optical output peaked between about 750 nm to 1150 nm.
3. The method of claim 1 , wherein the laser system has a heat spreader.
4. The method of claim 1 , further comprises a polarizer.
5. The method of claim 4 , wherein the polarizer is within the laser resonator.
6. The method of claim 1 , wherein the pump bias current is modified based on characterized thermal performance and thermal variation.
7. The method of claim 1 , wherein the pump source has optical output peaked between about 1450 nm to 1600 nm.
8. The method of claim 1 , wherein the pump source has optical output peaked between about 1800 nm to 2100 nm.
9. The method of claim 1 , wherein the pumping source resonantly pumps the RE:XAB gain medium with optical output having a peak wavelength within 200 nm of the laser system's emission wavelength.
10. The method of claim 1 , wherein the laser system further comprises a photodetector, the photodetector detecting pulse emissions.
11. The method of claim 10 , wherein the pump bias current profile is modified based on temporal feedback from the photodiode.
12. The method system of claim 10 , wherein the photodiode is an avalanche photodiode.
13. The method of claim 1 , wherein the current profile reduces pulse-to-pulse jitter.
14. The method of claim 1 , wherein the pump pulse is temporally shorter than the excited state lifetimes of the RE:XAB gain medium.
15. The method of claim 1 , wherein the current profile is operated for asynchronous pulse frequency operation.
16. The method of claim 1 wherein the current profile is a superposition of a plurality of pump sources.
17. The method of claim 1 , wherein the RE:XAB gain medium is double-end pumped.
18. The method of claim 17 , wherein at least one of the plurality of pump sources have different emission wavelengths than another of the plurality of pump sources.
19. The method of claim 17 , wherein the pump pulse is a plurality of pulses.
20. The method of claim 3 , wherein the laser system has an optically transparent heat spreader.
21. The methods 20 , wherein the optically transparent heat spreader is sapphire or synthetic diamond.