dc.creator |
Young, Mitchell E. |
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dc.creator |
Short, C. Ian (Christopher Ian), 1965- |
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dc.date.accessioned |
2018-04-05T12:29:38Z |
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dc.date.available |
2018-04-05T12:29:38Z |
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dc.date.issued |
2014-05-20 |
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dc.identifier.issn |
0004-637X |
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dc.identifier.uri |
http://library2.smu.ca/handle/01/27396 |
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dc.description |
Publisher's Version/PDF |
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dc.description.abstract |
Spectra for two-dimensional (2D) stars in the 1.5D approximation are created from synthetic spectra of one-dimensional (1D) non-local thermodynamic equilibrium (NLTE) spherical model atmospheres produced by the PHOENIX code. The 1.5D stars have the spatially averaged Rayleigh–Jeans flux of a K3–4 III star while varying the temperature difference between the two 1D component models (ΔT<sub>1.5D</sub>) and the relative surface area covered. Synthetic observable quantities from the 1.5D stars are fitted with quantities from NLTE and local thermodynamic equilibrium (LTE) 1D models to assess the errors in inferred T<sub>eff</sub> values from assuming horizontal homogeneity and LTE. Five different quantities are fit to determine the T<sub>eff</sub> of the 1.5D stars: UBVRI photometric colors, absolute surface flux spectral energy distributions (SEDs), relative SEDs, continuum normalized spectra, and TiO band profiles. In all cases except the TiO band profiles, the inferred T<sub>eff</sub> value increases with increasing ΔT<sub>1.5D</sub>. In all cases, the inferred T<sub>eff</sub> value from fitting 1D LTE quantities is higher than from fitting 1D NLTE quantities and is approximately constant as a function of ΔT<sub>1.5D</sub> within each case. The difference between LTE and NLTE for the TiO bands is caused indirectly by the NLTE temperature structure of the upper atmosphere, as the bands are computed in LTE. We conclude that the difference between T<sub>eff</sub> values derived from NLTE and LTE modeling is relatively insensitive to the degree of the horizontal inhomogeneity of the star being modeled and largely depends on the observable quantity being fit. |
en_CA |
dc.description.provenance |
Submitted by Betty McEachern (betty.mceachern@smu.ca) on 2018-04-05T12:29:38Z
No. of bitstreams: 1
Young_Mitchell_E_article_2014.pdf: 1212414 bytes, checksum: 655bb199495fe740421adb897663f303 (MD5) |
en |
dc.description.provenance |
Made available in DSpace on 2018-04-05T12:29:38Z (GMT). No. of bitstreams: 1
Young_Mitchell_E_article_2014.pdf: 1212414 bytes, checksum: 655bb199495fe740421adb897663f303 (MD5)
Previous issue date: 2014-05-20 |
en |
dc.language.iso |
en |
en_CA |
dc.publisher |
IOP Publishing |
en_CA |
dc.relation.uri |
https://dx.doi.org/10.1088/0004-637X/787/1/43 |
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dc.rights |
Article is made available in accordance with the publisher’s policy and is subject to copyright law. Please refer to the publisher’s site. Any re-use of this article is to be in accordance with the publisher’s copyright policy. This posting is in no way granting any permission for re-use to the reader/user. |
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dc.subject.lcsh |
Red giants |
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dc.subject.lcsh |
Stars -- Atmospheres |
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dc.subject.lcsh |
Cool stars |
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dc.subject.lcsh |
Astronomical photometry |
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dc.subject.lcsh |
Astronomical spectroscopy |
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dc.title |
Non-local thermodynamic equilibrium 1.5D modeling of red giant stars |
en_CA |
dc.type |
Text |
en_CA |
dcterms.bibliographicCitation |
Astrophysical Journal 787(1), 43. (2014) |
en_CA |