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Fig. 9

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Gap radius, Rgap, with respect to the accretion rate, M˙$\[\dot{M}_{\star}\]$, (‘Rgap M˙$\[R_{\text {gap }}-\dot{M}_{\star}\]$’-wall) for the models from Table 2 that trigger accretion events. The cyan dots represent observational data taken from Ercolano & Pascucci (2017) (labelled as ‘E+2017’). To indicate the possible range of our models, we added two additional models: ‘gap_large’ and ‘gap_small’. The models ‘gap_large’ and ‘gap_small’ have initial accretion rates of M˙init =3×108Myr1$\[\dot{M}_{\text {init }}=3 \times 10^{-8} ~M_{\odot} \mathrm{~yr}^{-1}\]$ and M˙init =109Myr1$\[\dot{M}_{\text {init }}=10^{-9} ~M_{\odot} \mathrm{~yr}^{-1}\]$ and X-ray luminosities of 1030 erg s−1 and 1029 erg s−1 were assumed, respectively. These models range from small accretion rates and small gap sizes in the lower-left corner to large gap sizes with accretion rates of ≲3 × 10−9 M yr−1 (lower-right side of the plot).

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