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Fig. 3

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Distribution of micro-turbulence for models with solar abundances for different effective temperatures Teff and surface gravities log   g (colour-coded). We had to disable the convection for the giants with Teff ≳ 5500 K and therefore no micro-turbulence was applied to these spectra. In and around this area we observe numerical instabilities causing single models to show differing results. Over-plotted are observational data points taken from Landstreet et al. (2009) (+) and Takeda et al. (2008) (×).

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