2014
DOI: 10.1088/1742-6596/511/1/012064
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Characterization of a laser plasma produced from a graphite target

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Cited by 6 publications
(3 citation statements)
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“…Besides, C II (wavelength 426.7, 514.6, and 589.1 nm), 31 and CN (wavelength 388.3, 359 and 421.6 nm) 29 are observed on the spectra. The C II emission lines are commonly observed in the methane working gas.…”
Section: Resultsmentioning
confidence: 93%
“…Besides, C II (wavelength 426.7, 514.6, and 589.1 nm), 31 and CN (wavelength 388.3, 359 and 421.6 nm) 29 are observed on the spectra. The C II emission lines are commonly observed in the methane working gas.…”
Section: Resultsmentioning
confidence: 93%
“…For Larmor radius effects to be relevant in determining the plasma dynamics, the ion Larmor radius has to be at least of the order of the characteristic linear dimensions of the laser-magnetic field interaction volume. Although no direct measurements of the plasma temperature have been performed in these experiments, by using available data from graphite targets, using the same laser parameters and background conditions as reported here, 32 or similar ones available in the literature, 21,[33][34][35] the ion Larmor radius for the average magnetic field strength in this case is estimated to be of the order of a few millimeters. As this value is about one tenth of the characteristic linear dimensions of the plasma expansion volume, two finite Larmor radius effects are expected to influence plasma behavior.…”
Section: Aip Advances 7 085002 (2017)mentioning
confidence: 99%
“…Such transient plasmas play a significant role in the production of various nanostructured materials (carbon nanotubes, nanowires, graphene, etc.) [11][12][13], and controlling their properties (expansion velocities, density, and temperature) allows a significant enhancement of the deposition process [14][15][16].…”
Section: Introductionmentioning
confidence: 99%