Table 4.
Scaling relation parameters at the 68% c.l. when varying the EoS for dark energy.
| Experiment | BM, 0 | α | σlnM | β |
|---|---|---|---|---|
| Euclid-like, 1% SR, T08 | 0.0 ± 0.001 | 0.0 ± 0.0020 |
 |
 |
| Euclid-like, 5% SR, T08 | 0.0 ± 0.005 | 0.0 ± 0.010 | 0.2002 ± 0.0084 |
 |
| Euclid-like, 5% SR, D16 | −0.0007 ± 0.0047 | 0.002 ± 0.010 | 0.1935 ± 0.0088 | 0.1250 ± 0.0034 |
| Euclid-like, 10% SR, T08 | 0.0 ± 0.010 | 0.0 ± 0.020 | 0.201 ± 0.015 | 0.1245 ± 0.0051 |
| LSST-like, 1% SR, T08 | 0.0 ± 0.0011 | 0.0 ± 0.0019 | 0.2001 ± 0.0018 | 0.1250 ± 0.0011 |
| LSST-like, 5% SR, T08 | 0.0 ± 0.0047 | 0.001 ± 0.010 | 0.1995 ± 0.0087 |
 |
| LSST-like, 10% SR, T08 | 0.0 ± 0.010 | 0.0 ± 0.019 | 0.201 ± 0.015 | 0.1248 ± 0.0064 |
| WFIRST-like, 1% SR, T08 | 0.0 ± 0.0010 |
 |
 |
0.1250 ± 0.0013 |
| WFIRST-like, 5% SR, T08 | 0.0 ± 0.0049 | 0.0 ± 0.010 | 0.200 ± 0.010 | 0.1249 ± 0.0053 |
| WFIRST-like, 10% SR, T08 | 0.0 ± 0.010 | 0.0 ± 0.019 | 0.200 ± 0.018 | 0.1249 ± 0.0077 |
Notes. We report results for the Euclid-like, LSST-like, and WFIRST-like simulated experiments at different levels of scaling relation precision. We show the comparison between the T08 and D16 mass function formulations only for the Euclid-like experiment.
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