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Fig. 6

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Gap-opening efficiency factor G, normalized to the adiabatic 2D model value Gadb2D$G_{{\rm{adb}}}^{2{\rm{D}}}$, as a function of the cooling timescale β for our fully radiative models (green) and those with local, β cooling (purple), finding a good agreement between 2D and 3D models. Local β cooling overestimates G compared to fully radiative models.

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