2009
DOI: 10.1364/ol.34.001894
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Pulse compression of submillijoule few-optical-cycle infrared laser pulses using chirped mirrors

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Cited by 22 publications
(11 citation statements)
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References 19 publications
(23 reference statements)
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“…9 In this letter, we demonstrate the generation of 0.4 mJ 11.5 fs laser pulses at 1.8 m. Similar to our recent work using the OPA Signal wavelength, 9 we spectrally broaden the Idler via nonlinear propagation in a HCF. Instead of chirped mirrors or adaptive devices for dispersion compensation, we show that laser pulses can be efficiently compressed utilizing solely the properties of fused silica ͑FS͒ in the anomalous dispersion regime below the third order dispersion ͑TOD͒ limit of bulk material.…”
supporting
confidence: 67%
“…9 In this letter, we demonstrate the generation of 0.4 mJ 11.5 fs laser pulses at 1.8 m. Similar to our recent work using the OPA Signal wavelength, 9 we spectrally broaden the Idler via nonlinear propagation in a HCF. Instead of chirped mirrors or adaptive devices for dispersion compensation, we show that laser pulses can be efficiently compressed utilizing solely the properties of fused silica ͑FS͒ in the anomalous dispersion regime below the third order dispersion ͑TOD͒ limit of bulk material.…”
supporting
confidence: 67%
“…Experiments were performed at the Advanced Laser Light Source (ALLS) at INRS-EMT using a Ti:Sapphire laser (Thales, 100 Hz, 80 mJ, 30 fs), which is described in [9,10]. The wavelength of the laser is shifted with an optical parametric amplifier (Light Conversion TOPAS-HE), broadened in a gas filled hollow fiber and then compressed with either chirped mirrors at 1.4 μm [11] or anomalous dispersion in fused silica glass at 1.8 μm [7]. The 7 mm diameter laser beam is focused with a 250 mm focal length spherical mirror, with an approximate f-number of 35.…”
Section: Methodsmentioning
confidence: 99%
“…Over the past decade, several pulse-compression techniques based on phase modulation induced by nonlinear optical effects have been developed extensively. One of the important methods to obtain compressed pulse is using self-phase modulation (SPM) in a gas-filled hollow fiber [1,2], a filament in gas cell [3,4], a fiber [5], or a bulk medium [6,7] to broaden spectrum and then compensating the spectral phase dispersion. This method is usually used to generate intense few-cycle pulses.…”
Section: Introductionmentioning
confidence: 99%