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Fig. C.1.

image

Left and middle panels: radial (ξr(R)) and horizontal (ξh(R)) components of the Lagrangian displacement vectors. Right panel: rotational kernels and the Brunt–Väisälä frequency (N) in the near-core region in which the g modes have the highest probing power. These displacement vectors and kernels are of the lowest and highest radial order modes of the theoretical period-spacing pattern of our overall best model (M = 1.65 M, Xc = 0.24, fov = 0.005, and log Dmix = 1.5). A full derivation of these quantities is provided in Unno et al. (1989) and Aerts et al. (2010).

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