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Fig. 4

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(a) Time evolution of the normalized maximal deviation from the azimuthally averaged surface density distribution for various numerical configurations. Inadequate resolution in the R-direction can damp the viscous instability, with convergence being achieved for our fiducial model with NR = 465. (b) Comparison of the same quantity for different azimuthal resolutions and NR = 465. The higher resolution of Nϕ = 1300 azimuthal cells results in square grid cells but does not influence the growth of the instability.

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