Fig. 5
Differences in μHz between observed GOLF frequencies used for sound speed inversion (Turck-Chièze & Lopes 2012) and theoretical frequencies of the SSM scaled by the inertia ratio Qn,l using MLT convection (diamonds); the Canuto prescription of convection (triangles; Canuto & Mazzitelli 1991); the mean thermal description (crosses); and 3D simulations from (Nordlund & Stein 1998; squares). See also Piau et al. (2014) for the results obtained with the MDI data.
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