2007
DOI: 10.1364/ao.46.004032
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Spontaneous emission from the C3 radical in carbon plasma

Abstract: Spontaneous emission measurements are discussed for the Swings transitions of the C(3) radical in laser-generated graphite plasma, and the spectroscopy of the C(3) radical in carbon vapor and plasma is summarized. A review is given of some theoretical calculations and emission spectroscopic investigations are presented. Time-averaged, laser-induced optical breakdown spectra are reported from Nd:YAG laser generated graphite microplasma. In 200-300 Torr of argon and helium, and depending on the specific experime… Show more

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Cited by 31 publications
(18 citation statements)
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“…The weakness of C 3 emissions in our spectra is somewhat surprising as it has been known for a long time that the C 3 radical is a dominant component of thermal equilibrium carbon vapors [29]. Some likely explanations for the weak emissions can be found by considering nonequilibrium conditions [30], electron collision cross-sections [31,32] and C 3 cation formation [33] and slow intersystem crossing from triplet C 3 to singlet C 3 [34] in laser ablation plasma.…”
Section: Discussion Of Experimentsmentioning
confidence: 84%
“…The weakness of C 3 emissions in our spectra is somewhat surprising as it has been known for a long time that the C 3 radical is a dominant component of thermal equilibrium carbon vapors [29]. Some likely explanations for the weak emissions can be found by considering nonequilibrium conditions [30], electron collision cross-sections [31,32] and C 3 cation formation [33] and slow intersystem crossing from triplet C 3 to singlet C 3 [34] in laser ablation plasma.…”
Section: Discussion Of Experimentsmentioning
confidence: 84%
“…Emission of 40 nm diameter particles reaches a maximum at near 550-600 nm [16]. There are two other sources, which could contribute to the observed continuum, either linear carbon molecules (C n with n≥4) or PAHs.…”
Section: Plasma Emission Spectroscopymentioning
confidence: 99%
“…23 C 3 is also the predominant carbon cluster in equilibrium hot carbon vapor, 19,24 hydrocarbon flames, 2,19 and plasmas generated through energetic processing of carbon containing materials. 19,25,26 The relevance of the C 3 molecule in space 27 as well as in terrestrial sooting flames and combustion processes 2,19 has motivated many experimental [28][29][30] and theoretical 17,18,[31][32][33][34][35][36][37][38][39][40][41] ) electronic manifolds. 23,[38][39][40] It is worth pointing out that, from the theoretical perspective, much effort has been devoted to obtain local (near-equilibrium) ground state potential energy surfaces 42 (PESs) for C 3 aiming to explore its spectroscopy, notably the unusual large amplitude bending motion and related speculations concerning its quasi-linearity (for a comprehensive review, see Refs.…”
Section: Introductionmentioning
confidence: 99%