1989
DOI: 10.1364/ol.14.000039
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Enhanced mode locking of color-center lasers

Abstract: A significant enhancement in the mode locking of a KCl:Tl color-center laser has been observed when a length of optical fiber having positive group-velocity dispersion was incorporated within an external control cavity. Pulse durations of ~260 fsec were obtained by this method, representing a compression factor ~60x that with the colorcenter laser alone. Similar results have also been observed with an InGaAsP semiconductor diode amplifier as the nonlinear element within the control cavity.

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Cited by 163 publications
(6 citation statements)
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“…Today in solid-state lasers, dyes have either demonstrated for a case where no soliton effects \vere present (22). In this case, an uncompressed pulse was fed back into the main cavity.…”
Section: Saturable Absorbers and Passive Mode-lockingmentioning
confidence: 99%
“…Today in solid-state lasers, dyes have either demonstrated for a case where no soliton effects \vere present (22). In this case, an uncompressed pulse was fed back into the main cavity.…”
Section: Saturable Absorbers and Passive Mode-lockingmentioning
confidence: 99%
“…This work led to the accidental discovery of additive pulse modelocking (APM) because the "wrong" fiber with positive instead of negative GDD was used inside a coupled cavity but stable modelocking was still observed in 1989 [55]. This was initially a puzzling result because generally a pulse becomes broadened after propagating in a fiber with positive dispersion.…”
Section: Coupled-cavity Modelockingmentioning
confidence: 99%
“…This approach exploits the intensitydependent phase profile of figure 6(a) and thus produces an intensity-dependent loss-the requirement for passive mode-locking. The technique is called Coupled Cavity Mode-locking (CCM) [30] or Additive Pulse Mode-locking (APM) [31]. This approach was first demonstrated as early as 1984 [32] but, after intensive refinement, it is rarely used in bulk solid-state lasers owing to the requirement to stabilize the differential pathlength of the interferometer to better than one wavelength.…”
Section: (T) Is the Phase Delay As A Function Of Time Experienced Bymentioning
confidence: 99%