2005
DOI: 10.1063/1.2159576
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Time-resolved dynamics of resonant and nonresonant broadband picosecond coherent anti-Stokes Raman scattering signals

Abstract: Published by the AIP PublishingArticles you may be interested in Analysis of time resolved femtosecond and femtosecond/picosecond coherent anti-Stokes Raman spectroscopy: Application to toluene and Rhodamine 6G

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Cited by 88 publications
(69 citation statements)
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References 11 publications
(9 reference statements)
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“…Recent advances in the microscopic applications of this technique have improved signal collection through the use of tightly focused beams 2 which relax the phase matching condition, and techniques for limiting the non-resonant signal. 3,4 Spectroscopic studies have separated resonant from non-resonant signal in the time-domain 3 and designed more efficient 5,6 collection sequences. The enhancement of CARS by intense plasmon fields could potentially enhance signal further and is the motivation for this work.…”
mentioning
confidence: 99%
“…Recent advances in the microscopic applications of this technique have improved signal collection through the use of tightly focused beams 2 which relax the phase matching condition, and techniques for limiting the non-resonant signal. 3,4 Spectroscopic studies have separated resonant from non-resonant signal in the time-domain 3 and designed more efficient 5,6 collection sequences. The enhancement of CARS by intense plasmon fields could potentially enhance signal further and is the motivation for this work.…”
mentioning
confidence: 99%
“…1, and the ps-CARS optical setup has been described in detail previously. 17 Briefly, it consists of a ps-duration, pulsed Nd:YAG laser (Ekspla, Model SL230) that operates at 10 Hz and produces nearly transform-limited pulses [fullwidth-at-half-maximum (FWHM) duration of $150 ps and maximum pulse energy of 100 mJ/pulse] at 532 nm; this beam is split into pump and probe beams, each with an energy of 800 lJ/pulse. A fraction of this laser output is also split off to pump a home-made modeless dye laser (FWHM bandwidth of $5 nm and FWHM duration of $110 ps) for generating the Stokes beam at 606 nm with an energy of 3 mJ/pulse.…”
Section: Methodsmentioning
confidence: 99%
“…We have applied picosecond coherent anti-Stokes Raman scattering (ps-CARS), which is a well-established non-invasive approach to measuring temperature in a reacting environment with excellent accuracy and precision, [16][17][18][19] to allow thermometric measurements of the gas-phase species in thermal equilibrium with reacting, energetic nanoparticle samples following laser flash heating. This point-wise detection approach permits spatially resolved measurements under single-laser-shot conditions, and the temporal resolution of this approach is limited only by the greater of the durations of the flash-heating laser [several nanoseconds (ns) in this work] and the sub-ns pulse durations used in the ps-CARS techniques.…”
Section: Introductionmentioning
confidence: 99%
“…Such a variation in temperature would normally be accompanied by a factor of several hundred reduction in signal intensity in rotational CARS measurements. 19 However, by taking advantage of the significantly larger coherence dephasing rates encountered in lower temperature gas zones as opposed to high temperature zones, 21,22 a probe delay of 350 ps brings the CARS signal levels from both hot zones and cold zones to within a factor of 20 of each other, well within the 16-bit dynamic range of a typical CCD.…”
Section: (Right)mentioning
confidence: 99%