2012
DOI: 10.1364/oe.20.018732
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Characterization of broadband few-cycle laser pulses with the d-scan technique

Abstract: We present an analysis and demonstration of few-cycle ultrashort laser pulse characterization using second-harmonic dispersion scans and numerical phase retrieval algorithms. The sensitivity and robustness of this technique with respect to noise, measurement bandwidth and complexity of the measured pulses is discussed through numerical examples and experimental results. Using this technique, we successfully demonstrate the characterization of few-cycle pulses with complex and structured spectra generated from … Show more

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Cited by 200 publications
(170 citation statements)
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“…Pulses from a Femtopower Compact Pro amplifier were compressed to 5-fs duration and 750-μJ pulse energy using self-phase modulation in a neon-filled (2-bar) hollow-core fiber and a chirped mirror compressor (optics from Ultrafast Innovations). The compressed pulses had a continuous spectrum spanning from 400 to 1,000 nm and were characterized using dispersion scan [Sphere Photonics (51)] to have a duration of 4.9 fs. The 1-kHz repetition rate was reduced to 100 Hz using an optical chopper to avoid sample damage, and the beam was split into two arms using an 80-20% broadband beam splitter.…”
Section: Methodsmentioning
confidence: 99%
“…Pulses from a Femtopower Compact Pro amplifier were compressed to 5-fs duration and 750-μJ pulse energy using self-phase modulation in a neon-filled (2-bar) hollow-core fiber and a chirped mirror compressor (optics from Ultrafast Innovations). The compressed pulses had a continuous spectrum spanning from 400 to 1,000 nm and were characterized using dispersion scan [Sphere Photonics (51)] to have a duration of 4.9 fs. The 1-kHz repetition rate was reduced to 100 Hz using an optical chopper to avoid sample damage, and the beam was split into two arms using an 80-20% broadband beam splitter.…”
Section: Methodsmentioning
confidence: 99%
“…The pulses are characterized online using an integrated dscan device directly under vacuum [14]. At optimal compression, we generate 3.5fs pulses (1.3 cycle at 750nm central wavelength) with 3.5mJ energy, corresponding to 1TW peak power.…”
Section: Futurementioning
confidence: 99%
“…This necessarily means that they are insensitive to time-invariant parameters of the field. The well-established methods of the past two decades, including FROG [11], SPIDER [12], MIIPS [13], and D-Scan [14], have played important roles in the development of ultrafast laser sources and for characterizing laser pulses used in a wide range of experiments. However, they suffer from a number of limitations in their capabilities: (i) they measure only the spectral/temporal intensity and dispersion/chirp, not the full electric field, including the carrier-envelope phase (CEP); (ii) they cannot measure the relative phase across spectral nulls without an auxiliary field with a bandwidth that spans the null [15,16]; (iii) for ultrabroad bandwidth pulses, the bandwidth and efficiency of the measurement is limited by the requirement to use a nonlinear material to act as a time-stationary filter; and (iv) the pulse is rarely measured in situ, which necessitates a careful calibration of the linear and nonlinear space-time propagation of the pulse from the diagnostic to the site of the experiment.…”
Section: Introductionmentioning
confidence: 99%