1991
DOI: 10.1103/physreva.44.7134
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Radiative lifetimes in Si i from laser-induced fluorescence in the visible, ultraviolet, and vacuum ultraviolet

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Cited by 59 publications
(23 citation statements)
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“…Our g f value for the Si i line at 3905 8 is that of NIST, which is taken from the laboratory work of Garz (1973). This is close to the value of À1.04 dex given by O'Brian & Lawler (1991), whose work is focused on the UV and hence do not reach redder than 4110 8. They report only an upper limit to the gf value for the 4103 8 line of Si i for which Cayrel et al (2003) adopt a log g f value of À3.14 dex ( F. Spite 2004, private communication), again taken from the 1973 study.…”
Section: Comparison With Cayrel Et Al (2003)supporting
confidence: 53%
“…Our g f value for the Si i line at 3905 8 is that of NIST, which is taken from the laboratory work of Garz (1973). This is close to the value of À1.04 dex given by O'Brian & Lawler (1991), whose work is focused on the UV and hence do not reach redder than 4110 8. They report only an upper limit to the gf value for the 4103 8 line of Si i for which Cayrel et al (2003) adopt a log g f value of À3.14 dex ( F. Spite 2004, private communication), again taken from the 1973 study.…”
Section: Comparison With Cayrel Et Al (2003)supporting
confidence: 53%
“…One clear example of such a correction are the oscillator strengths of Si I lines provided by Garz (1975) [10], which were later rescaled by O'Brian and Lawler (1991) [11]. Not only do the majority of rescaled values produce great agreement with the Paper 2 results, but they also show substantial improvements in the median offsets compared to the unscaled sources.…”
Section: Comparisons Between the Brass Results And Previously Retrievsupporting
confidence: 65%
“…References with lines belonging to several species are denoted with *. [20,21] Fe I 3 0.010 0.014 Sobeck et al (2007) [22] Cr I 14 0.020 0.055 Kostyk (1982a) [17] Ti I 7 0.020 0.018 Garz (1973) rescaled using O'Brian and Lawler (1991) [10,11] Si I 7 0.020 0.033 Blackwell et al (1986) rescaled using Grevesse et al (1989) [23,24] Ti I 3 0.020 0.037 Kostyk (1982b) [18] Ni Lennard et al (1975) [30] Ni I 3 0.050 0.087 Kostyk (1981) [16] Cr I 6 0.050 0.016 Smith and O'Neill (1975) [31] Ca I 3 0.050 0.026 Blackwell et al (1979) [32] Fe I 3 0.050 0.029 Ryabchikova et al (1999) [33] Fe II 3 0.050 0.049 Martin et al (1988) [34] Cr [41] Ni I 3 0.080 0.038 Blackwell et al (1986) [23] Ti I 12 0.080 0.037 May et al (1974) [42] Fe I 82 0.080 0.096 Kostyk and Orlova (1983) [43] Cr II/Ti II 3 0.090 0.074 Blackwell et al (1980) [44] Fe II 9 0.100 0.131 Kurucz and Bell (1995) [45] Si I 7 0.100 0.033 Garz (1973) [10] Si I 7 0.100 0.033 Wiese and Martin (1990) [46] * 25 0.100 0.243 Fuhr et al (1988) [47] Fe I/Ni I 112 0.100 0.116 …”
Section: Comparisons Between the Brass Results And Previously Retrievmentioning
confidence: 99%
“…Comparison of the present data with the measurements of O'Brian and Lawler [4] provides an accurate indicator of the overall uncertainties in the theoretical calculations. We find that the overall agreement between the two sets of data for the 26 fine structure transitions reported is within 5-10%, with the exception of some very weak transitions, e.g.…”
Section: Resultsmentioning
confidence: 74%
“…The fine structure ƒ-values, obtained from the length form, are then compared individually with the experimental values. The calculated and measured A-values are also given for Si I. Si I experimental data are reported by O'Brian and Lawler [4], who have measured a number of transitions using laser-induced fluorescence technique which apparently has very low uncertainties, and by Becker et al [5] who used beam-foil technique. The error bars for measured values of Si I by O'Brian and Lawler are approximate since they have been converted from ±logR 10 R (gf).…”
Section: Resultsmentioning
confidence: 99%