Figure 10.
As in Fig. 8, but applying the correction factor $f_{\Delta \nu } = (\Delta \nu _{\mathrm{obs}}/\sqrt{\rho _{\mathrm{surf}}})$ and $f_{\nu _{\mathrm{max}}}$. The corresponding model for each star was obtained from interpolating the observed $\Delta \nu$ into the isochrone’s surface corrected $\Delta \nu$ sequence. Additionally, a red-clump-specific correction factor $f_{\nu _{\mathrm{max}}} = 1.0477$ has been applied. The mean red giant and mean red clump values from the four different equations show excellent agreement among them.

As in Fig. 8, but applying the correction factor |$f_{\Delta \nu } = (\Delta \nu _{\mathrm{obs}}/\sqrt{\rho _{\mathrm{surf}}})$| and |$f_{\nu _{\mathrm{max}}}$|⁠. The corresponding model for each star was obtained from interpolating the observed |$\Delta \nu$| into the isochrone’s surface corrected |$\Delta \nu$| sequence. Additionally, a red-clump-specific correction factor |$f_{\nu _{\mathrm{max}}} = 1.0477$| has been applied. The mean red giant and mean red clump values from the four different equations show excellent agreement among them.

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