Bibcode
Ramírez, I.; Allende Prieto, C.; Redfield, S.; Lambert, D. L.
Bibliographical reference
Astronomy and Astrophysics, Volume 459, Issue 2, November IV 2006, pp.613-625
Advertised on:
11
2006
Journal
Citations
25
Refereed citations
23
Description
The atmospheric parameters and iron abundance of the Sloan Digital Sky
Survey (SDSS) spectrophotometric standard star BD +17 4708 are
critically examined using up-to-date Kurucz model atmospheres, LTE line
formation calculations, and reliable atomic data. We find
Teff=6141 ± 50 K, log g=3.87 ± 0.08, and
[Fe/H]=-1.74 ± 0.09. The line-of-sight interstellar reddening,
bolometric flux, limb-darkened angular diameter, stellar mass, and the
abundances of Mg, Si, and Ca are also obtained: E(B-V)=0.010 ±
0.003, fbol=(4.89±0.10) × 10-9 erg
cm-2 s-1, θ=0.1016 ± 0.0023 mas,
M=0.91 ± 0.06~M_&sun;, [Mg/Fe]=0.40 ± 0.10, [Si/Fe]=0.35
± 0.11, [Ca/Fe]=0.36 ± 0.11. This star is a unique example
of a moderately metal-poor star for which the effective temperature
(Teff) can be accurately constrained from the observed
spectral energy distribution (corrected for reddening). Such analysis
leads to a value that is higher than most spectroscopic results
previously reported in the literature (~5950 K). Interstellar reddening
was estimated using various prescriptions, including an analysis of
interstellar lines. The surface gravity of the star was inferred from
the fitting of the wings of the Mg I b lines. We used transition
probabilities measured in the laboratory and reliable damping constants
for unblended Fe lines to derive the iron abundance using both Fe I and
Fe II lines. We find that the ionization balance of Fe lines is
satisfied only if a low Teff (~5950 K) is adopted. The mean
iron abundance we obtain from the Fe II lines corresponds to A_Fe=5.77
± 0.09 ([Fe/H]=-1.74 for our derived AFe,&sun;=7.51)
while that from the Fe I lines is A_Fe=5.92 ± 0.11, and therefore
with our preferred Teff (6141 K), the discrepancy between the
mean iron abundance from Fe I and Fe II lines cannot be explained by
overionization by UV photons as the main non-LTE effect. Interestingly,
the Fe I excitation balance is satisfied with a Teff only
slightly warmer than our preferred solution and not with the lower value
of 5950 K. We also comment on non-LTE effects and the importance of
inelastic collisions with neutral H atoms in the determination of oxygen
abundances in metal-poor stars from the 7774 Å O I triplet.