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Table 9

Stellar parameters and abundances for the 6 (non-Mira, non-symbiotic) Henize S stars with HERMES high-resolution spectra available.

Low-resolution High-resolution Difference
Hen 4- T eff log g [Fe/H] C/O [Zr/Fe]a [Fe/H] C/O [Zr/Fe] Δ[Fe/H] ΔC/O Δ[Zr/Fe]



134 3600 0. –0.5 0.50 +0.92 −0.41 ± 0.18 0.65 ± 0.15 1.22 ± 0.27 –0.09 –0.15 –0.30
147 3700 1. +0.0 0.50 +0.92 −0.09 ± 0.13 0.55 ± 0.11 1.17 ± 0.21 0.09 –0.05 –0.25
174 3500 1. –0.5 0.75 +0.92 −0.42 ± 0.20 0.56 ± 0.12 1.39 ± 0.27 –0.08 0.19 –0.47
191 3200 0. –0.5 0.90 +0.92 −0.49 ± 0.14 0.90 ± 0.05 1.03 ± 0.33 –0.01 0.00 –0.11
193 3600 1. –0.5 0.75 +0.92 −0.44 ± 0.17 0.63 ± 0.14 0.87 ± 0.22 –0.06 0.12 0.05
196 3500 1. –0.5 0.50 +0.92 −0.43 ± 0.18 0.54 ± 0.11 1.15 ± 0.33 –0.07 –0.04 –0.23

Notes. The data in Cols. 2–6 are the parameters characterizing the atmospheric models selected by the BMF procedure operating solely on photometry and low-resolution spectra (in fact: “degraded” high-resolution spectra, see text), whereas abundances in Cols. 7–9 are derived from the high-resolution HERMES spectra. The last three columns provide the differences between low-resolution and high-resolution abundances.

(a)

The grid models selected for these 6 stars all have an s-process enrichment of [s/Fe] = +1, but setting [s/Fe] = +1 in MARCS and Turbospectrum results in [Zr/Fe] = +0.92, because of the (weak) r-contribution to the solar system Zr.

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