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Fig. 2

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Steady-state gas density in the belt (in Keplerian motion) as predicted by our model for different values of gas production rate. The line in red represents ncrit which is the critical density below which the gas has a wind structure (see Eq. (5)) for collisions between SW protons and either C, O, or ions. Above this critical density, the gas is assumed to form a viscous disk with α = 10−3. The case of high Msw = 105 shows the regime where tleave/thit > 1, independent of Ṁsw where we assume υsw = 100 km/s (see main text for details).

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