Table 3.
Cosmological parameters at the 68% c.l. when varying the EoS for dark energy.
| Experiment | Ωm | σ8 | w0 | wa |
|---|---|---|---|---|
| Euclid-like, 1% SR, T08 | 0.3164 ± 0.0013 | 0.8121 ± 0.0012 |
 |
 |
| Euclid-like, 5% SR, T08 | 0.3165 ± 0.0018 | 0.8122 ± 0.0033 | −1.000 ± 0.010 |
 |
| Euclid-like, 5% SR, D16 | 0.3066 ± 0.0020 | 0.8153 ± 0.0034 | −1.095 ± 0.012 |
 |
| Euclid-like, 10% SR, T08 | 0.3163 ± 0.0027 | 0.8121 ± 0.0051 |
 |
 |
| LSST-like, 1% SR, T08 |  |
 |
−1.003 ± 0.010 |
 |
| LSST-like, 5% SR, T08 | 0.3167 ± 0.0020 |
 |
−1.000 ± 0.012 |
 |
| LSST-like, 10% SR, T08 | 0.3165 ± 0.0030 | 0.8118 ± 0.0050 | −1.000 ± 0.014 |
 |
| WFIRST-like, 1% SR, T08 |
 |
0.8342 ± 0.0036 | −1.000 ± 0.015 |
 |
| WFIRST-like, 5% SR, T08 | 0.3169 ± 0.0038 | 0.8119 ± 0.0050 | −0.998 ± 0.021 |
 |
| WFIRST-like, 10% SR, T08 | 0.3167 ± 0.0044 | 0.8122 ± 0.0079 | −0.999 ± 0.024 |  |
Notes. We report the 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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