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Intracavity second harmonic generation

II. Intracavity Second Harmonic Generation Using an Organic Crystal... [Pg.223]

We have recently conducted a set of intracavity second harmonic generation experiments using the organic nonlinear material DAN (4-(N,N-dimethylamino)-3-acetamidonitrobenzcne) and an optically pumped cw Nd YAG laser (2). Figure 3 shows the experimental setup. Quasi-cw operation was achieved with crystal samples immersed in index matching fluid in an antireflection coated cuvette that was placed internal to the Nd YAG laser cavity. [Pg.223]

K. M. Gheri, C. Saavedra, D. F. Walls. Intracavity second-harmonic generation using an electromagnetically induced transparency. Physical Revew A 1993 May 4 48(4) 3344-3361. [Pg.98]

V. Petrov, D. Georgiev, and U. Stamm, Improved Mode Locking of a Femtosecond Titanium-Doped Sapphire Laser by Intracavity Second Harmonic Generation , Appl. Phys. Lett. 60, 1550 (1992). [Pg.191]

Fig. 20. Schematic diagram of the Synchroscan streak camera system. A Spectra Physics model 164 acousto-optically mode-locked argon ion laser modulated at 69.44MHz pumps the Rhodamine 6G dye laser formed by mirrors Mi, M2, M3 and M4. This dye laser typically produces pulses of 2 ps duration with an energy content of 0.6 nJ. The second harmonic is generated intracavity in an ADP crystal. The UV radiation is then coupled out through mirror Ms and a filter F2 is used to eliminate any transmitted visible light before focusing into the sample cell with lens Lt. The fluorescence is detected at 90 to the incident beam. A lens L2 collects the fluorescence which passes through a polarizer and a bandpass filter and then onto the slit of the streak camera. (After ref. 69.)... Fig. 20. Schematic diagram of the Synchroscan streak camera system. A Spectra Physics model 164 acousto-optically mode-locked argon ion laser modulated at 69.44MHz pumps the Rhodamine 6G dye laser formed by mirrors Mi, M2, M3 and M4. This dye laser typically produces pulses of 2 ps duration with an energy content of 0.6 nJ. The second harmonic is generated intracavity in an ADP crystal. The UV radiation is then coupled out through mirror Ms and a filter F2 is used to eliminate any transmitted visible light before focusing into the sample cell with lens Lt. The fluorescence is detected at 90 to the incident beam. A lens L2 collects the fluorescence which passes through a polarizer and a bandpass filter and then onto the slit of the streak camera. (After ref. 69.)...

See other pages where Intracavity second harmonic generation is mentioned: [Pg.219]    [Pg.223]    [Pg.88]    [Pg.219]    [Pg.223]    [Pg.88]    [Pg.81]    [Pg.108]    [Pg.156]    [Pg.156]    [Pg.21]    [Pg.579]    [Pg.134]    [Pg.19]    [Pg.579]    [Pg.83]   
See also in sourсe #XX -- [ Pg.220 , Pg.221 ]




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