Table 3.
Amplitudes of 2D CFs of LCDM models.
Sample | ρ0 | 1 | 2 | 4 | 8 | 16 | 32 | 64 | 2048 | 3D |
---|---|---|---|---|---|---|---|---|---|---|
512 | 256 | 128 | 64 | 32 | 16 | 8 | 0.25 | |||
LCDM.00 | 0 | 0.0280 | 0.0540 | 0.1084 | 0.198 | 0.329 | 0.481 | 0.617 | 0.717 | 0.722 |
LCDM.01 | 1 | 0.0461 | 0.0889 | 0.1784 | 0.326 | 0.541 | 0.792 | 1.017 | 1.185 | 1.191 |
LCDM.02 | 2 | 0.0579 | 0.1117 | 0.224 | 0.412 | 0.683 | 1.000 | 1.289 | 1.505 | 1.515 |
LCDM.05 | 5 | 0.0764 | 0.1477 | 0.297 | 0.549 | 0.910 | 1.336 | 1.730 | 2.017 | 2.039 |
LCDM.10 | 10 | 0.0917 | 0.1781 | 0.358 | 0.667 | 1.105 | 1.620 | 2.105 | 2.430 | 2.478 |
LCDM.20 | 20 | 0.1092 | 0.212 | 0.430 | 0.810 | 1.337 | 1.961 | 2.558 | 2.933 | 2.986 |
LCDM.50 | 50 | 0.1356 | 0.275 | 0.574 | 1.106 | 1.803 | 2.644 | 3.467 | 3.811 | 3.954 |
Notes. Table columns starting from the left: sample name, particle-density limit ρ0, 2D CF amplitudes, A = ξ(6) for sample parameter n = 1, 2, 4, 8, 16, 32, 64, 2048. The last column gives amplitudes from the 3D analysis. In the table head, the upper line gives n, and the next line gives sheet thickness L = 512/n in h−1 Mpc.
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