Emission characteristics and dynamics of C 2 from laser produced graphite plasma. Harilal, S., S., Issac, R., C., Bindhu, C., V., Nampoori, V., P., N., & Vallabhan, C., P., G. 81(April):3637-3643, 1997. abstract bibtex The emission features of laser ablated graphite plume generated in a helium ambient atmosphere have been investigated with time and space resolved plasma diagnostic technique. Time resolved optical emission spectroscopy is employed to reveal the velocity distribution of different species ejected during ablation. At lower values of laser fluences only a slowly propagating component of C 2 is seen. At high fluences emission from C 2 shows a twin peak distribution in time. The formation of an emission peak with diminished time delay giving an energetic peak at higher laser fluences is attributed to many body recombination. It is also observed that these double peaks get modified into triple peak time of flight distribution at distances greater than 16 mm from the target. The occurrence of multiple peaks in the C 2 emission is mainly due to the delays caused from the different formation mechanism of C 2 species. The velocity distribution of the faster peak exhibits an oscillating character with distance from the target surface.
@article{
title = {Emission characteristics and dynamics of C 2 from laser produced graphite plasma},
type = {article},
year = {1997},
pages = {3637-3643},
volume = {81},
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abstract = {The emission features of laser ablated graphite plume generated in a helium ambient atmosphere have been investigated with time and space resolved plasma diagnostic technique. Time resolved optical emission spectroscopy is employed to reveal the velocity distribution of different species ejected during ablation. At lower values of laser fluences only a slowly propagating component of C 2 is seen. At high fluences emission from C 2 shows a twin peak distribution in time. The formation of an emission peak with diminished time delay giving an energetic peak at higher laser fluences is attributed to many body recombination. It is also observed that these double peaks get modified into triple peak time of flight distribution at distances greater than 16 mm from the target. The occurrence of multiple peaks in the C 2 emission is mainly due to the delays caused from the different formation mechanism of C 2 species. The velocity distribution of the faster peak exhibits an oscillating character with distance from the target surface.},
bibtype = {article},
author = {Harilal, S S and Issac, Riju C and Bindhu, C V and Nampoori, V P N and Vallabhan, C P G},
number = {April}
}
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