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Table A.3.
Mean logarithmic density gradients, aI − IV, of our models at a given collapse.
| Model | # | aI | aII | aIII | aIV |
|---|---|---|---|---|---|
| e-10k | 0.60 ± 0.22 | 2.39 ± 0.26 | 2.32 ± 0.07 | 3.44 ± 0.03 | |
| e-50k | 1st | 0.56 ± 0.21 | 2.41 ± 0.03 | 2.27 ± 0.03 | 3.36 ± 0.01 |
| 2nd | 0.61 ± 0.15 | 2.37 ± 0.12 | 2.19 ± 0.02 | 3.35 ± 0.01 | |
| m-20k | 1st | 0.17 ± 0.21 | 2.09 ± 0.60 | 1.60 ± 0.10 | 3.96 ± 0.08 |
| 2nd | 0.12 ± 0.24 | 2.07 ± 0.68 | 1.70 ± 0.09 | 3.89 ± 0.11 | |
| 3rd | 0.12 ± 0.24 | 2.22 ± 0.64 | 1.68 ± 0.08 | 3.80 ± 0.10 | |
| m-100k | 1st | 0.26 ± 0.31 | 1.76 ± 0.24 | 1.53 ± 0.18 | 3.97 ± 0.07 |
| 2nd | 0.64 ± 0.25 | 1.88 ± 0.60 | 1.64 ± 0.10 | 3.85 ± 0.12 | |
| 3rd | 0.47 ± 0.16 | 1.95 ± 0.21 | 1.63 ± 0.06 | 3.61 ± 0.10 |
Notes. The fitted radii where the power law breaks, rI − III, shown in Table A.4. All numbers are given with their 1σ deviations calculated from the corresponding number of realisations.
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