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Table 3.
Expected contributions to the observed scatters for the Redge–mass and Σedge–mass relations due to different observational errors.
| z | σR, mass | σΣ, mass | σR, size | σΣ, size | σR, int | σΣ, int |
|---|---|---|---|---|---|---|
| Chamba et al. (z ∼ 0.1) | 0.05 ± 0.01 | – | 0.07 ± 0.01 | – | 0.04 ± 0.01 | 0.27 ± 0.02 |
| 0.1 < z < 0.3 | 0.04 ± 0.01 | 0.09 ± 0.01 | 0.03 ± 0.01 | 0.19 ± 0.02 | 0.10 ± 0.01 | 0.29 ± 0.04 |
| 0.3 < z < 0.5 | 0.04 ± 0.01 | 0.09 ± 0.01 | 0.03 ± 0.01 | 0.16 ± 0.01 | 0.09 ± 0.01 | 0.28 ± 0.02 |
| 0.5 < z < 0.7 | 0.04 ± 0.01 | 0.09 ± 0.01 | 0.03 ± 0.01 | 0.15 ± 0.01 | 0.10 ± 0.01 | 0.31 ± 0.02 |
| 0.7 < z < 0.9 | 0.04 ± 0.01 | 0.09 ± 0.01 | 0.03 ± 0.01 | 0.15 ± 0.01 | 0.09 ± 0.01 | 0.24 ± 0.01 |
| 0.9 < z < 1.1 | 0.04 ± 0.01 | 0.09 ± 0.01 | 0.04 ± 0.01 | 0.19 ± 0.01 | 0.11 ± 0.01 | 0.31 ± 0.02 |
Notes. We also include the expected intrinsic scatters of the observed relations (σR, int and σΣ, int) once they are corrected of the observational uncertainties.
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