Abstract
The conditions for optimum 611.8 nm laser operation are obtained and a convenient method for indicating 3.39 µm suppression is proposed. Single longitudinal mode 611.8 nm generation is obtained using higher gas-mixture pressure and application of an axial magnetic field. Several milliwatt monomode output power and 0.75 multimode-to-monomode power conversion coefficients are obtained without an internal iodine cell. A comparison of the experimental results with a single-mode laser theory is given.
Article PDF
Similar content being viewed by others
Avoid common mistakes on your manuscript.
References
M. Glaser: Metrologia 23, 45 (1986); IEEE TIM-36, 2, 604 (1987)
M.V. Danileyko, A.M. Tselinko, L.P. Yatsenko: Kvant. electr. (Sov.) 9, 11, 2346 (1982)
A.P. Voytovich, I.L. Katsev: Zh. Prikl. Spectr. (Sov.) 3, 38 (1965)
W. Luhs, B. Struve, G. Litfin: Laser and Optoelektron. 18, 319 (1986)
Ya.M. Bondarchuk et al.: Opt. Spektrosk. 64, 6, 1377 (1988)
Ya.M. Bondarchuk et al.: Opt. Spektrosk. 62, 5, 1196 (1987)
E.G. Saprikin, R.N. Yudin, S.N. Atutov: Opt. Spektrosk. 34, 755 (1973)
St.St. Cartaleva, S.V. Gateva, G.V. Kolarov: Appl. Phys. B 40, 153 (1986)
S.N. Atutov, S.N. Selesnev, A.M. Shalagin: Zh. Prikl. Spectr. (Sov.) 31, 6, 977 (1979)
Yu.V. Troitskiy: Single Frequency Gas Lasers (Nauka, Novosibirsk 1975)
V.I. Fadeev, N.M. Terent'ev: Possibility Functions (Moscow 1954)
P.W. Smith, T. Hansch: Phys. Rev. Lett. 26, 740 (1971)