Abstract
Due to spatial hole burning, standing-wave dye lasers require a large amount of selectivity inside the cavity for single-mode operation. The output power of these lasers is limited by losses caused by the frequency selecting elements. In a travelling-wave laser, on the other hand, spatial hole burning does not exist, thereby eliminating the need for high selectivity. A travelling-wave cw dye laser was realized by unidirectional operation of a ring laser, yielding single mode output powers of 1.2 W at 595 nm and of 55 mW in the UV-region with intracavity frequency doubling.
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References
C. T.Pike: Opt. Commun.10, 14 (1974)
G.Marowsky, K.Kaufmann. IEEE J. Quant. Electr. QE-12, 207 (1976)
H. W.Schröder, H.Dux, H.Welling: Appl. Phys.7, 21 (1975)
I.v.Hertel, A. S.Stamatović: IEEE J. Quant. Electr. QE-11, 210 (1975)
D.Frölich, L.Stein, H. W.Schröder, H.Welling: Appl. Phys.11, 97 (1976)
J. M.Green, J. P.Hohimer, F. K.Tittel: Opt. Commun.7, 349 (1973)
C. L.Tang, H.Statz, G.de Mars: Appl. Phys. Lett.2, 222 (1963)
M.Sargent: Appl. Phys.9, 127 (1976)
J. B.Hambenne, M.Sargent: IEEE J. Quant. Electr. QE-11, 90 (1975)
C. L.O'Bryan, M.Sargent: Phys. Rev. A-8, 3071 (1973)
G.Marowsky: Appl. Phys. Lett.26, 647 (1975)
M.Hercher, M.Young, C. B.Smoyer. J. Appl. Phys.36, 3351 (1965)
A. A.Mak, V. I.Ustyugov, V. A.Fromzel', M. M.Khaleev: Sov. Phys.-Tech. Phys.19, 552 (1974)
B. B.Snavely: Continuous-Wave Dye Lasers, inDye Lasers, ed. by F. P.Schäfer, Top. Appl. Phys., Vol.1 (Springer, Berlin, Heidelberg, New York 1973 or 1977)