2010
DOI: 10.1080/00268971003627824
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Spontaneous emission from C2(d3Πg) and C3(A1Πu) during laser irradiation of soot particles

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Cited by 39 publications
(22 citation statements)
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“…There is strong evidence in the literature to support this explanation for the secondary enhancement of light attenuation. A major product of the laser-induced sublimation of carbon is C 3 [33,34,35,36,37] which has strong Swings bands absorption near 405 nm [38,39,40] and can explain the secondary enhancement observed in the present work at 405 nm. Swan band absorption of C 2 radicals, formed in substantial amounts upon sublimation of soot [41,42,43,36,44], has a peak near 474 nm and may contribute to the secondary enhancement of 488-nm light attenuation observed in the present work.…”
Section: The Diffusion Flamesupporting
confidence: 51%
“…There is strong evidence in the literature to support this explanation for the secondary enhancement of light attenuation. A major product of the laser-induced sublimation of carbon is C 3 [33,34,35,36,37] which has strong Swings bands absorption near 405 nm [38,39,40] and can explain the secondary enhancement observed in the present work at 405 nm. Swan band absorption of C 2 radicals, formed in substantial amounts upon sublimation of soot [41,42,43,36,44], has a peak near 474 nm and may contribute to the secondary enhancement of 488-nm light attenuation observed in the present work.…”
Section: The Diffusion Flamesupporting
confidence: 51%
“…The signal-to-noise ratio is found higher in Flame1.95 due to the higher number density of incipient soot. The C 2 emission can be identified at high laser fluences (Goulay et al 2010). When C 2 emission is clearly visible, the spectral ranges considered for the fitting were reduced to two narrower spectral ranges, i.e., [450-500 nm] and [525-800 nm] to exclude the interference of C 2 emission.…”
Section: Results and Discussion: LII Measurements And Modelingmentioning
confidence: 99%
“…In addition, there are other factors that can have an influence on LII signals and signal decay rates, including aggregate size [243][244][245][246][247][248][249][250][251][252], aggregate morphology [244,253], polydispersity of primary-particle size [250][251][252][254][255][256][257], and soot-maturity effects on thermal-accommodation coefficients [99,190]. In addition, detection wavelengths must be selected carefully to avoid numerous potential interferences [258,259]. Nevertheless, considerable work performed by many members of the LII community has led to great advances in improving the utility of this technique under a wide range of conditions.…”
Section: Laser-induced Incandescencementioning
confidence: 99%