Fig. 3.

Thorough force resolution analysis of the three-dimensional projected density ρ(x) for a three sine wave initial set-up with ϵ = (3/4, 1/2). A subcube of size L/10 is extracted from the snapshot corresponding to expansion factor a = 0.04 and sampled with 5123 voxels. The nature of the run (Vlasov or PM) and its parameters are detailed in each panel, in particular the spatial resolution ng of the grid used to solve the Poisson equation. In addition, the resolution ns of the mesh of vertices employed to construct the initial tessellation is indicated for the Vlasov runs and its analogue np for the network of particles in the PM simulations, along with the value of the refinement control parameter I for Vlasov. The spatial resolution scale εr = L/ng represents about 1/102 of the subcube size in the upper right panel; 1/51 in the middle top panel and second row of panels; and 1/26, then 1/13 in the next two rows of panels. For completeness (from top to bottom and left to right), the runs considered are designated respectively as VLA-ANI2-HR, VLA-ANI2-MR, VLA-ANI2-LR, VLA-ANI2-HRS, VLA-ANI2-FHR, VLA-ANI2-MRa, VLA-ANI2-LRa, PM-ANI2-UHR, PM-ANI2-HR, PM-ANI2-MR, and PM-ANI2-LR in Table 1.
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