2002ApJ...573..662S


Query : 2002ApJ...573..662S

2002ApJ...573..662S - Astrophys. J., 573, 662-669 (2002/July-2)

Gas-phase iron abundances and depletions in translucent interstellar lines of sight from far ultraviolet spectroscopic explorer observations of Fe II lines.

SNOW T.P., RACHFORD B.L. and FIGOSKI L.

Abstract (from CDS):

Far Ultraviolet Spectroscopic Explorer (FUSE) wavelength coverage includes several weak- to moderate-strength lines of Fe II, allowing the determination, through curve-of-growth analysis, of accurate Fe II abundances and hence iron depletions. We have analyzed Fe II absorption lines toward 18 of the reddened stars included in the FUSE survey of molecular hydrogen abundances in translucent clouds. Our analysis is based on equivalent width measurements and curves of growth, aided by the fact that some of the observed lines are weak enough to be on the linear part of the curve of growth. In interpreting our abundance and depletion results, we have combined our data with those of an earlier survey of interstellar iron abundances and depletions in diffuse clouds, based on Copernicus data. The principal result of our survey is that iron depletions, known from earlier work to increase with average line-of-sight density for diffuse clouds, do not continue to increase with either density or extinction in translucent clouds; i.e., there is no significant trend of increasing depletion with increasing extinction or molecular fraction. This may be due to the fact that our data set does not probe lines of sight with greater average volume densities than those that were covered by the previous Copernicus-based survey of iron depletions. We conclude by reevaluating the definition of translucent clouds, based on the lack of enhanced iron depletions in our sample.

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Journal keyword(s): ISM: Dust, Extinction - ISM: Abundances - ISM: Molecules

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* X Per HXB 03 55 23.0777456088 +31 02 45.039836148 6.090 6.840 6.720     O9.5III 1037 0
2 * 62 Tau * 04 23 59.7627483096 +24 18 03.527065188 6.18 6.499 6.337     B3V 237 0
3 HD 62542 * 07 42 37.2147724128 -42 13 47.831717064   8.21 8.03     B3V 164 0
4 HD 73882 ** 08 39 09.53412 -40 25 09.2608 7.07 7.59 7.19 6.67 6.30 O8.5IV 261 1
5 HD 110432 HXB 12 42 50.2663572384 -63 03 31.052981412 4.79 5.58 5.31     B0.5IVpe 334 0
6 HD 154368 s*b 17 06 28.3687759224 -35 27 03.760593156 6.10 6.63 6.13 7.12   O9.5Iab 316 0
7 HD 167971 s*b 18 18 05.8947362832 -12 14 33.313601112 7.89 8.27 7.50 6.68 6.279 O8Iaf(n)+O4/5 324 0
8 HD 168076 Y*O 18 18 36.4205083536 -13 48 02.420915796 8.12 8.72 8.25 7.62 7.21 O4III(f) 209 0
9 HD 170740 SB* 18 31 25.6939245072 -10 47 45.008376432 5.51 5.96 5.72     B2V+ 210 1
10 HD 185418 * 19 38 27.4809937872 +17 15 26.048161044 7 7.639 7.485     B0.5V 144 0
11 HD 192639 s*b 20 14 30.4275801672 +37 21 13.816276704 6.83 7.46 7.11     O7.5Iabf 309 0
12 HD 197512 * 20 42 10.0488399504 +49 44 05.060333040 7.93 8.60 8.55     B1V 70 0
13 HD 199579 Y*O 20 56 34.7779063080 +44 55 29.000891928 5.16 6.01 5.96     O6.5V((f))z 375 0
14 HD 203938 ** 21 23 50.1690416971 +47 09 52.446883103 7.13 7.54 7.08     B0.5IV 108 0
15 HD 206267 Y*O 21 38 57.6195772032 +57 29 20.554016280 5.09 5.83 5.62   5.56 O6.0V((f))+O9:V 520 0
16 HD 207198 Y*? 21 44 53.2791389640 +62 27 38.048647248 5.61 6.25 5.94 5.66 5.49 O8.5II 365 0
17 HD 207538 * 21 47 39.7896725544 +59 42 01.348647696 7 7.55 7.30     O9.7IV 213 1
18 * lam Cep s*b 22 11 30.5765111040 +59 24 52.154264880 4.55 5.29 5.05 4.77 4.62 O6.5I(n)fp 705 1

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