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Passive mode-locking of dye lasers

dye laser can also be passively mode-locked and two different arrangements have been used. The first employed two free flowing dye streams, one for the laser dye and the other for the absorber (see Fig. 4) [18, 19]. In the alternative arrangement, the saturable absorber dye flows in a narrow channel of variable thickness (0.2—0.5mm) and in contact with a 100% broadband reflectivity mirror. With an absorber thickness of 0.5 mm, output pulses of 1 ps duration have been obtained [20]. Pulses as short as 0.3ps were produced when the DODCI cell length was shortened to 0.2 mm. The subpicosecond pulses produced in this arrangement were transform-limited in bandwidth. [Pg.7]

In summary, the laser provides the photochemist with a light source which is powerful, directional, monochromatic, and possibly tunable. The beam can be on continuously, or pulsed with pulse widths as short as a few picoseconds. [Pg.7]

output pulses of 1 ps duration have been obtained [20]. Pulses as short as 0.3ps were produced when the DODCI cell length was shortened to 0.2 mm. The subpicosecond pulses produced in this arrangement were transform-limited in bandwidth. [Pg.7]


See other pages where Passive mode-locking of dye lasers is mentioned: [Pg.6]    [Pg.6]   


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LASER locking

Lasers modes

Mode locking

Mode passive

Of dyes

Of passivity

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