2000
DOI: 10.1007/s003400000483
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Femtosecond ultraviolet pulses generated using noncollinear optical parametric amplification and sum frequency mixing

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Cited by 23 publications
(8 citation statements)
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“…Electronic excitation was achieved with pulses (336 nm, 1.7 m̈J, 60 fs) generated by the sum frequency mixing of the fundamental of a standard 1 kHz amplified Ti:sapphire laser (Spitfire, Spectra Physics) and visible pulses generated by a noncollinear optical parametric amplifier 46 . After passing an optical delay line, the pump pulses were focused onto the sample with a beam diameter of approximately 300 m̈m.…”
Section: Methodsmentioning
confidence: 99%
“…Electronic excitation was achieved with pulses (336 nm, 1.7 m̈J, 60 fs) generated by the sum frequency mixing of the fundamental of a standard 1 kHz amplified Ti:sapphire laser (Spitfire, Spectra Physics) and visible pulses generated by a noncollinear optical parametric amplifier 46 . After passing an optical delay line, the pump pulses were focused onto the sample with a beam diameter of approximately 300 m̈m.…”
Section: Methodsmentioning
confidence: 99%
“…We excited a 100 mm thick jet or a home-built rotating sample cell consisting of 1 mm thick CaF 2 windows with a 100 mm thick teflon spacer containing the sample solutions with the second harmonic of a home built 1 kHz amplified Ti:sapphire laser system (wavelength 400 nm, pulse duration 55 fs, energy 3-7 mJ, spot diameter 200 mm) or with pulses centred at 350 nm (pulse duration 50 fs, energy 1-3 mJ, same spot diameter) generated by sum-frequency mixing of the fundamental with visible pulses obtained with a noncollinear parametric amplifier. [47] Tunable mid-infrared probe pulses of 100-150 fs duration were generated by difference frequency mixing of signal and idler pulses from a near-infrared optical parametric amplifier. [48] After spectral dispersion with a polychromator the probe pulses were detected by a multichannel detector for the mid-IR.…”
Section: Methodsmentioning
confidence: 99%
“…They indeed generate tuneable pulses that can be finely varied over the entire visible region and straightforwardly extended into the UV by frequency doubling or upconverting with a powerful IR pulse. 18,19 These arrangements result in 30-50 fs pulses with typically 0.1-1 mJ energy and tuning from 250 to 350 nm. 20,21 Ultrafast transient absorption One of the first works where the NOPA's flexibility was exploited to investigate a chemical process was carried out by Schenkl et al in 2005.…”
Section: State Of the Art: Methodologiesmentioning
confidence: 99%