Table 1.
Parameters of the three simulations analyzed in this article.
Designation | ϵ2D | ng | ns | ai | aSC, x | aSC, y | aℳ | ar | |
---|---|---|---|---|---|---|---|---|---|
Q1D | 1/6 | 2048 | 2048 | 0.005 | 0.05285 | 0.14 | 0.2 | 0.26 | |
ANI | 2/3 | 2048 | 2048 | 0.005 | 0.04545 | 0.055 | 0.1 | 0.125 | |
SYM | 1 | 2048 | 2048 | 0.005 | 0.04090 | 0.04090 | 0.055 | 0.075 |
Notes. All three simulations have been performed assuming a matter-dominated Universe ΩM = 1 and starting expansion factor aini = 0.0005. The second column gives the relative amplitude of the sine waves along the x and y axes: ϵ2D=ϵy/ϵx. ng denotes the spatial resolution of the grid over which the Poisson equation is solved and ns denotes the spatial resolution of the grid used for tessellation. ai is the expansion factor of the first output snapshot, whose mass profile Mi we measure and scale our self-similar solutions accordingly. aSC, x, aSC, y are the estimated expansion factors at first shell-crossings along the x and y axes, respectively. aℳ, ar are the expansion factors of the earliest snapshots for which self-similar fits to the mass profile and the particle trajectories could converge.
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