Table F.1.
All inferred cosmological and astrophysical parameters varied within the anisotropic systematics and the standard isotropic systematics models from the KiDS-1000 gold sample.
SBI: anisotropic sys. | SBI: std. isotropic sys. | MCMC: anisotropic sys. | MCMC: std. isotropic sys. | |||||
---|---|---|---|---|---|---|---|---|
Marginal | MAP | Marginal | MAP | Marginal | MAP | Marginal | MAP | |
±1σ | ±PJ-HPD | ±1σ | ±PJ-HPD | ±1σ | ±PJ-HPD | ±1σ | ±PJ-HPD | |
S8 | 0.731 ± 0.033 |
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0.770 ± 0.029 |
σ8 |
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Ωm |
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h0 |
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— |
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— |
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ωc |
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ωb |
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0.0225 ± 0.0020 |
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— |
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— | 0.0225 ± 0.0019 |
ns |
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— |
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AIA |
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Abary |
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> 2.45 |
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> 2.48 |
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Notes. The columns marked with SBI show the constraint obtained from the KiDS-SBI analaysis, while the columns marked with MCMC represent the parameter constraints obtained from a standard MCMC analysis which assumes a Gaussian likelihood with a sample covariance matrix derived from the respective forward model. The second, fourth, sixth and seventh columns show the mean marginals as well as the upper and lower 68% confidence intervals, i.e. 1σ, of the marginals. The third and fifth columns show the maximum a posteriori (MAP), and the uncertainties are defined as the upper and lower 68% confidence intervals, i.e. 1σ, given by the projected joint highest posterior density, PJ-HPD (Robert 2007; Joachimi et al. 2021).
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