2000
DOI: 10.1007/s003400000288
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Generation of 8-fs pulses at 390 nm

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Cited by 18 publications
(12 citation statements)
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“…The origin of the rapidly varying spectral features is not fully understood but is not necessarily the QPM nature of the device, since a similar behavior was observed with birefringent phase matching. 3 We observed no indications of two-photon absorption or self-phase-modulation in the CPPLT.…”
mentioning
confidence: 52%
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“…The origin of the rapidly varying spectral features is not fully understood but is not necessarily the QPM nature of the device, since a similar behavior was observed with birefringent phase matching. 3 We observed no indications of two-photon absorption or self-phase-modulation in the CPPLT.…”
mentioning
confidence: 52%
“…2) and 8 fs (Ref. 3) were generated by doubling of ϳ10-fs pulses from a Ti:sapphire oscillator by use of birefringent phase matching. In the latter experiment, focusing the FH tighter than confocally into a 100-mm-thick BBO crystal reduced the effective interaction length and alleviated SH pulse broadening owing to GVM.…”
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confidence: 99%
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“…The nearly transform-limited pulse is then focused onto a 100-µm thick BBO crystal with a spherical mirror (f = 12mm) as discussed by Furbach et al, providing SH light with approximately 3 mW average power and a large spectral bandwidth (Figure 2d). 8 The probe beam is then directed to a second home-built pulse shaping setup using a SLM (Boulder Nonlinear Systems) in order to compensate for the dispersion of the microscope objective. Work to optimize the chirp of the probe beam is ongoing.…”
Section: Imaging Systemsmentioning
confidence: 99%
“…For example, Furbach et al directly upconverted a high-power Ti:Sapph oscillator in a bulk doubling crystal [17]. Their model, based on standard plane-wave interactions, could not explain the rapid structure of their spectrum or its bandwidth.…”
Section: Downloaded By [The Agamentioning
confidence: 99%