Fig. 5
Abundance pattern of HIP 56948 (circles) versus condensation temperature. The solid line represents the mean abundance pattern. The error bars are based only on the observational uncertainties, which are ~0.005 dex. The low element-to-element scatter from the fit for the volatile (σ = 0.004 dex) and refractory (σ = 0.007 dex) elements confirms the high precision of our work.
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