G Logan DesAutels et al 2003 J. Opt. A: Pure Appl. Opt. 5 96 doi:10.1088/1464-4258/5/2/304
G Logan DesAutels, Dan Daniels, John O Bagford and Mike Lander
Show affiliationsTwo methods of measuring the gain medium parameters of a laser are presented (Hodgson N and Weber H 1997 Optical Resonators–Fundamentals, Advanced Concepts and Applications (Berlin: Springer) pp 583–91). The first method used measured only the output power of the CO2 laser (10.6 μm is the wavelength used) using three separate output couplers, each having different couplings. Once the three different output powers were measured, the results were used in the Rigrod equation to solve for two separate Rigrod equations knowing all the variables except for two unknowns; the small signal gain coefficient and the saturation intensity. The second method was a single-pass measurement where a very low power CO2 laser was injected into the high power CO2 laser in question. Power readings were made before and after the injection to determine the gain. Both methods agree with each other well, within 5%, for the small signal gain calculation, which provides confidence that the calculation for saturation intensity in the first method is correct as well.
42.55.Lt Gas lasers including excimer and metal-vapor lasers
42.60.Jf Beam characteristics: profile, intensity, and power; spatial pattern formation
42.60.Lh Efficiency, stability, gain, and other operational parameters
Issue 2 (March 2003)
Received 15 April 2002, in final form 9 December 2002
Published 9 January 2003
G Logan DesAutels et al 2003 J. Opt. A: Pure Appl. Opt. 5 96
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