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Fig. 12

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Residuals of the subtraction of the eccentric theoretical model (left panels) and circular model (right panels) from the projected velocity in the simulation for i = 0° (top panels) and i = 30° (bottom panels). These maps were obtained assuming the upper emission surface to be =1 = 2.5H (as discussed in Sect. 5.3), and rescaling the simulations to have a binary with abin = 15 au, Mbin = 1 M, placed at a distance of d = 130 pc. Similarly to Fig. 9, we note that the convention about velocities in observations is that blue-shift of lines is associated with negative velocities, while red-shift is associated with positive velocities – for example, this implies that υz in this plot is opposite in sign with respect to that in Fig. 7. We note that the top right panel residual is obtained by subtracting υz,circ = 0 (as the circular case does not have vertical motion) from υz, thus this residuals map portrays the vertical velocity map on the τ = 1 surface for the case i = 0°. This highlights that the amplitude of the vertical oscillations reaches υz ~ 0.4 km s−1 in the upper emission layer.

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