1987
DOI: 10.1103/physreva.35.3033
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Radial profiles of ground-state transitions of heliumlike argon from the Alcator-Ctokamak

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Cited by 64 publications
(42 citation statements)
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“…These spectra, obtained for viewing chords tangent to r/a ∼ 0.9, include the resonance line, w (1s2p 1 P 1 -1s 2 1 S 0 , 3949.28 mÅ), the intercombination lines, x and y (1s2p 3 P 2 -1s 2 1 S 0 , 3965.99 mÅ, and 1s2p 3 P 1 -1s 2 1 S 0 , 3969.40 mÅ) and the forbidden line, z (1s2p 3 S 1 -1s 2 1 S 0 , 3994.28 mÅ). At the low electron temperatures of the edge plasma, the upper levels of these transitions were populated by radiative recombination of H-like argon [43], which was born at the plasma center, and was transported outward on the fast time scale of L-mode impurity confinement [44,45,46]. In the top frame, from an LOC plasma, the spectra from the top and bottom viewing chords have the same intensity, and it may be concluded that the edge impurity densities are up/down symmetric.…”
Section: Methodsmentioning
confidence: 99%
“…These spectra, obtained for viewing chords tangent to r/a ∼ 0.9, include the resonance line, w (1s2p 1 P 1 -1s 2 1 S 0 , 3949.28 mÅ), the intercombination lines, x and y (1s2p 3 P 2 -1s 2 1 S 0 , 3965.99 mÅ, and 1s2p 3 P 1 -1s 2 1 S 0 , 3969.40 mÅ) and the forbidden line, z (1s2p 3 S 1 -1s 2 1 S 0 , 3994.28 mÅ). At the low electron temperatures of the edge plasma, the upper levels of these transitions were populated by radiative recombination of H-like argon [43], which was born at the plasma center, and was transported outward on the fast time scale of L-mode impurity confinement [44,45,46]. In the top frame, from an LOC plasma, the spectra from the top and bottom viewing chords have the same intensity, and it may be concluded that the edge impurity densities are up/down symmetric.…”
Section: Methodsmentioning
confidence: 99%
“…Emission lines from the spectra of helium-like ions are often observed in the spectra of solar, stellar, and other astrophysical plasmas (Seely & Feldman 1985;Feldman et al 2000;Dere et al 2001;Ness et al 2003;Paerels & Kahn 2003;Phillips 2004;Landi & Phillips 2005;Güdel & Nazé 2009;. Spectral lines of helium-like ions are also prominent features in the X-ray spectra of tokamak and laser-produced plasmas (Hsuan et al 1987;Rice et al 1987Rice et al , 1999Rice et al , 2014Rice et al , 2015Beiersdorfer et al 1995). An analysis of spectral lines provides information on the temperature, density, and chemical composition of the plasma.…”
Section: Introductionmentioning
confidence: 99%
“…Spectral lines of helium-like ions are also prominent features in the X-ray spectra of tokamak plasmas and laser-produced plasmas. These features arise from impurity elements (e.g., Hsuan et al 1987;Bombarda et al 1988;Beiersdorfer et al 1995;Elton et al 2000;Rosmej et al 2002;Rice et al 1987Rice et al , 1999Rice et al , 2000Rice et al , 2014Rice et al , 2015. The relative intensities Full Tables 1 and 2 are only available at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/592/A141 of spectral lines from the n = 2 shell to the ground state have been widely used in temperature and density diagnostics for solar plasma (e.g., McKenzie et al 1979;Wolfson et al 1983;Keenan et al 1984;Doyle & Keenan 1986) and tokamak plasmas (e.g., Källne et al 1983;Keenan et al 1989).…”
Section: Introductionmentioning
confidence: 99%