Issue |
A&A
Volume 566, June 2014
|
|
---|---|---|
Article Number | A116 | |
Number of page(s) | 23 | |
Section | Stellar atmospheres | |
DOI | https://doi.org/10.1051/0004-6361/201423498 | |
Published online | 25 June 2014 |
Online material
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Fig. 1
FUSE spectrum of K 1−27 (gray) compared with final synthetic spectra (red: pure stellar, blue: combined stellar and interstellar). The locations of photospheric lines appearing in the synthetic spectrum are marked. |
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Fig. 1
continued. |
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Fig. 2
continued. |
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Fig. 3
Same as Fig. 1 for HS 1522+6615. |
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Fig. 3
continued. |
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Fig. 4
Same as Fig. 1 for HS 2209+8229. |
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Fig. 4
continued. |
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Fig. 5
HST/COS spectrum of K 1−27 (gray) compared with final synthetic spectra (red: pure stellar, blue: combined stellar and interstellar). The locations of photospheric (red) and interstellar (blue) lines reproduced by the synthetic spectrum are marked. |
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Fig. 7
Same as Fig. 5 for HS 1522+6615. |
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Fig. 8
Same as Fig. 5 for HS 2209+8229. |
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Fig. 9
Temperature, electron density stratification, and ionization fractions of all elements in our final model of K 1−27. |
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Fig. 11
Like Fig. 9, for HS 1522+6615. |
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Fig. 12
Like Fig. 9, for HS 2209+8229. |
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Fig. 21
Determination of the C abundance of HS 1522+6615. C iv lines are compared with models with different C abundances as indicated by the labels. |
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Fig. 22
Determination of the N abundance of K 1−27. N v lines in the EFOSC2 observation are compared with models with different N abundances as indicated by the labels. |
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Fig. 23
Determination of the O abundance of HS 2209+8229. O v and O vi lines are compared with models with different O abundances as indicated by the labels. |
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Statistics of the model atoms used in our TMAP calculations.
© ESO, 2014
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