New Journal of Physics · 2005 · 150 citations · 17 references
Natural SciencesPhysicsOpticsOptoelectronicsPhotonicsLaser OpticsLaser PhysicsNonlinear OpticsOscillatorsUltrafast OpticsAmplificationFemtosecond Laser PulsesLaser Pulse DurationMode-locked LasersSpectral Line BroadeningUltra-short Pulse GenerationUltrafast Pulse GenerationUltrashort Pulse Generation
Broadening the ultrashort laser pulse in a Kerr-lens mode-locked laser by net positive round-trip group-delay dispersion has proven to be a powerful concept for scaling the pulse energy directly achievable with a femtosecond laser oscillator without external amplification. Drawing on this concept, we demonstrate here Ti: Sa chirped-pulse oscillators delivering sub-40fs pulses of 0.5 μJ and 50 nJ energy at average power levels of 1 and 2.5 W (repetition rate: 2 and 50 MHz), respectively, which to the best of our knowledge constitute the highest pulse energy and average power achieved with a femtosecond (<100 fs) laser oscillator to date. The 0.5 μJ pulses have a peak power in excess of 10 MW and reach a peak intensity > 10 <sup>15</sup> W cm <sup>-2</sup> (when focused down to ∼1 μm <sup>2</sup>), both of which represent record values from a laser oscillator. These pulse parameters appear to be limited merely by the pump power available, affording promise of scaling chirped-pulse femtosecond Ti: Sa oscillators to microjoule pulse energies and - by simultaneous spectral broadening - towards peak power levels of several hundred megawatts. © IOP Publishing Ltd and Deutsche Physikalische Gesellschaft.
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Controlling the Phase Evolution of Few-Cycle Light Pulses
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Femtosecond solid-state lasers
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