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Fig. 5.

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Angular distribution of particles that become unbound between consecutive simulation snapshots, meaning the sums of their kinetic and potential energies become positive. The angle θ is the polar angle measured from z ˆ $ {\hat {{{\mathbf {z}}}}} $, which is the direction of the initial orbital angular momentum vector. Material is initially ejected near the orbital plane, then closer to the poles in single or double-sided outflows after the plunge-in.

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