2003
DOI: 10.1088/0022-3727/37/2/009
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An improved LTE model of a high pressure sulfur discharge

Abstract: An existing LTE model (Johnston C W et al 2002 J. Phys. D: Appl. Phys. 35 342) of a high pressure sulfur discharge is improved upon by more accurate and complete treatment of each term in the energy balance. The simulation program PLASIMO (Janssen G M et al 1999 Plasma Sources Sci. Technol. 8 1, van Dijk J 2001 Modelling of plasma light sources: an object-oriented approach PhD Thesis Eindhoven University of Technology, The Netherlands, ISBN 90-386-1819-0), which is an integrated environment for construction an… Show more

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Cited by 21 publications
(11 citation statements)
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(40 reference statements)
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“…14 Considerable effort has also gone toward the development of radiative-transfer models for these sulfur discharges. 15,16 The B − X system is the S 2 analog of the Schumann-Runge system in the isovalent O 2 molecule and has been the subject of numerous experimental and theoretical studies. In 32 S 2 , the v = 0-9 levels of the B state lie below the first dissociation limit.…”
Section: Introductionmentioning
confidence: 99%
“…14 Considerable effort has also gone toward the development of radiative-transfer models for these sulfur discharges. 15,16 The B − X system is the S 2 analog of the Schumann-Runge system in the isovalent O 2 molecule and has been the subject of numerous experimental and theoretical studies. In 32 S 2 , the v = 0-9 levels of the B state lie below the first dissociation limit.…”
Section: Introductionmentioning
confidence: 99%
“…In industrial condition, S 2 molecules can be seen in reactive ion etching process using SF 6 molecules [7]. Sulfur lamps contain S 2 molecules as an important ingredient [8]. Although electron collision with S 2 molecules is an important elementary process in these plasmas, there has been little work on this subject.…”
Section: Introductionmentioning
confidence: 99%
“…The optical thickness therefore increases extensively during the evaporation of sulfur, as it is expected, since the number density of the molecules in the vapor becomes much larger. When the steady regime is reached, the laser red spot cannot be distinguished anymore on the screen strongly illuminated by the white light coming from the plasma, confirming that its core in operating condition is optically thick (optical depth is about 10 µm according to [12]). In contrast, the vapor around the plasma core remains transparent, since one can see the rear grid through it.…”
Section: Observationsmentioning
confidence: 99%