1999
DOI: 10.1364/ol.24.000631
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Semiconductor saturable-absorber mirror–assisted Kerr-lens mode-locked Ti:sapphire laser producing pulses in the two-cycle regime

Abstract: Pulses of sub-6-fs duration have been obtained from a Kerr-lens mode-locked Ti:sapphire laser at a repetition rate of 100 MHz and an average power of 300 mW. Fitting an ideal sech(2) to the autocorrelation data yields a 4.8-fs pulse duration, whereas reconstruction of the pulse amplitude profile gives 5.8 fs. The pulse spectrum covers wavelengths from above 950 nm to below 630 nm, extending into the yellow beyond the gain bandwidth of Ti:sapphire. This improvement in bandwidth has been made possible by three k… Show more

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Cited by 374 publications
(180 citation statements)
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“…Ti:sapphire gain material has a particularly high optical gain bandwidth supporting less than 6-fs pulse duration from low energy oscillators [47,48], which is shorter than for any other laser materials. Unfortunately, its pump wavelength is in the blue-green spectral region, which requires complex and expensive pump lasers.…”
Section: Gain Materials With Larger Emission Bandwidthmentioning
confidence: 99%
“…Ti:sapphire gain material has a particularly high optical gain bandwidth supporting less than 6-fs pulse duration from low energy oscillators [47,48], which is shorter than for any other laser materials. Unfortunately, its pump wavelength is in the blue-green spectral region, which requires complex and expensive pump lasers.…”
Section: Gain Materials With Larger Emission Bandwidthmentioning
confidence: 99%
“…The titanium-doped sapphire crystal [7] as a gain material took over the role of dyes, since broader gain bandwidth, better thermal properties and convenient handling made femtosecond lasers simple and reliable light sources. However, the fundamentally different properties of this material required the invention of a new mode-locking technique [8], identified later as Kerr-lens mode-locking [9], which enabled the Ti:sapphire lasers to achieve the same record of pulse duration [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…One optical cycle at 800 nm is only 2.7 fs long. The long-standing record of 6-fs pulses [9] in the dye laser era in 1987 was passed for the first time in 1999, more than 10 years later, with a KLM SESAM-assisted Ti:sapphire laser using double-chirped mirrors (DCMs) for broadband dispersion compensation [10]. In contrast to the older world-record result no external pulse amplification and compression was necessary and these pulses were obtained directly at the output of the laser oscillator.…”
Section: Current Frontier In Klm Ti:sapphire Laser Oscillatorsmentioning
confidence: 99%
“…Because the Kerr lens produces a "nonresonant" saturable absorber, it is inherently broadband, broader than any other saturable absorber available today. Thus compared to the ultrafast dye lasers, for which only pulses as short as 27 fs with around 10 mW average power were generated [81], pulses around 5 to 6 fs with hundreds of milliwatts of average power can be produced with Ti:sapphire lasers [10,13]. In addition, very broad tunability with sub-100-fs pulses became possible for the first time.…”
Section: Kerr-lens Modelocking (Klm)mentioning
confidence: 99%