Abstract

When a Fabry-Perot is used for spectral narrowing in nitrogen laser pumped dye lasers their energy may be divided by ten. This is due to the nonstationary regime of the Fabry-Perot, which is analyzed in this paper by calculating the phase transmission vs time. Optimization of the spectral brightness through the choice of the reflectivity of the mirrors is calculated and compared to the experimental results in the uv range. The effect of the spacings of the mirrors on the integrated spectral resolution of the Fabry-Perot used as a spectrum analyzer is also looked at theoretically and experimentally.

© 1978 Optical Society of America

Efficient cavity dumped dye laser

R. G. Morton, M. E. Mack, and I. Itzkan
Appl. Opt. 17(20) 3268-3275 (1978)

Pressure-scanned three-pass Fabry-Perot interferometer

L. N. Durvasula and Robert W. Gammon
Appl. Opt. 17(20) 3298-3303 (1978)

Polarization of light from a pulsed dye laser

C. H. Dugan, A. Lee, and F. J. Morgan
Appl. Opt. 17(7) 1012-1014 (1978)

Generation of intense subnanosecond 0.58–0.80-μm pulses with a flashlamp-pumped dye laser

T. J. Negran and A. M. Glass
Appl. Opt. 17(17) 2812-2816 (1978)

Spectral characteristics of a short-pulse red–green–blue dye mixture laser

Yasunori Saito, Naoyuki Nakai, Akio Nomura, and Tetsuo Kano
Appl. Opt. 31(21) 4298-4304 (1992)