1955
DOI: 10.1051/jphysrad:01955001606049001
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Utilisation des étincelles glissantes pour l'analyse spectrale dans l'ultraviolet lointain. Possibilité de détection et dosage du soufre, du phosphore et du carbone dans les aciers

Abstract: Utilisation desétincelles glissantes pour l'analyse spectrale dans l'ultraviolet lointain. Possibilité de détection et dosage du soufre, du phosphore et du carbone dans les aciers.

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Cited by 12 publications
(3 citation statements)
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“…The exception is the C + 90.41 nm line, because the background continuum in this region is very low and the emission intensity of this line is relatively high (as shown in figure 4). The unprecedented detection limit of 87 ppm obtained from the 97.70 nm C 2+ line (compared to 100 ppm obtained by Balloffet and Romand [58] from the same line using the sliding vacuum spark technique) indicates that this line is the most sensitive carbon line in the VUV region, and therefore is the most suitable one for carrying out further quantitative analyses of metals and alloys to determine their carbon content. This detection limit could be further improved by carrying out other optimization procedures on different experimental parameters, for example ambient atmosphere and pressure; laser pulse energy and wavelength harmonics or by using a charge coupled device (CCD) detector which certainly provides a greater sensitivity and a better resolution.…”
Section: Limits Of Detectionmentioning
confidence: 74%
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“…The exception is the C + 90.41 nm line, because the background continuum in this region is very low and the emission intensity of this line is relatively high (as shown in figure 4). The unprecedented detection limit of 87 ppm obtained from the 97.70 nm C 2+ line (compared to 100 ppm obtained by Balloffet and Romand [58] from the same line using the sliding vacuum spark technique) indicates that this line is the most sensitive carbon line in the VUV region, and therefore is the most suitable one for carrying out further quantitative analyses of metals and alloys to determine their carbon content. This detection limit could be further improved by carrying out other optimization procedures on different experimental parameters, for example ambient atmosphere and pressure; laser pulse energy and wavelength harmonics or by using a charge coupled device (CCD) detector which certainly provides a greater sensitivity and a better resolution.…”
Section: Limits Of Detectionmentioning
confidence: 74%
“…The limits of detection for the five carbon lines are shown in table 4. Also in the table, for the C 2+ 97.70 nm line, a comparison is made with the only value available from the literature [58]. The limits of detection (c L ) in the present work were determined from the well known expression [65] c L = 3σ (I b )/S (6) where σ (I b ) is the standard deviation of measurements of the background intensity and S is the slope of the calibration curve for each relevant spectral line.…”
Section: Limits Of Detectionmentioning
confidence: 99%
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