Table 1.
Marginalised one-dimensional best-fitting parameters with 1σ confidence intervals for the simulated quasar sample 1 (2023 sources).
Model | ΩM | ΩΛ | γ | β | γ0 | γ1 | β0 | β1 |
---|---|---|---|---|---|---|---|---|
1 | 0.13 ± 0.07 | 0.43 ± 0.30 | 0.584 ± 0.011 | 8.44 ± 0.34 | – | – | – | – |
2 | 0.3 | 0.7 | 0.562 ± 0.009 | 9.08 ± 0.27 | – | – | – | – |
3 | 0.42 ± 0.28 | 0.68 ± 0.42 | – | – | 0.560 ± 0.032 | 0.010 ± 0.011 | 9.23 ± 0.98 | −0.33 ± 0.36 |
4 | 0.3 | 0.7 | – | – | 0.568 ± 0.026 | 0.007 ± 0.009 | 8.98 ± 0.80 | −0.23 ± 0.30 |
5 | 0.9 | 0.1 | 0.545 ± 0.009 | 9.49 ± 0.27 | – | – | – | – |
6 | 0.9 | 0.1 | – | – | 0.541 ± 0.027 | 0.015 ± 0.010 | 9.76 ± 0.83 | −0.51 ± 0.30 |
Notes. The simulation assumes γ = 0.6 and β = 8.0, with a dispersion of the LX − LUV relation of δ = 0.24. The distances have been computed assuming a spatially flat ΛCDM model with ΩM = 0.1 and ΩΛ = 0.9 (see Section 6 for details). The ΛCDM model has ΩM and ΩΛ free to vary for models 1 and 3, whilst models 2 and 4 have the matter and energy parameters fixed to the values 0.3 and 0.7, respectively. Models 3 and 4 assume an evolution with redshift of both slope and intercept of the X-ray to UV relation in the form: γ(z) = γ0 + γ1(1 + z) and β(z) = β0 + β1(1 + z). In all models, Ωk is fixed to zero (spatially flat case) and Ωr = 2.47 × 10−5 h−2, with h = 0.7 km s−1 Mpc−1, Ωr = 1 − ΩM − ΩΛ, and ΩΛ < 0.99 + 1.8 ΩM. The latter condition has been enforced to exclude solutions with no Big Bang. Models 5 and 6 are the same as 2 and 4, respectively, but with matter and energy parameter values fixed to ΩM = 0.9 and ΩΛ = 0.1. Model 3 is a sanity check to test what happens when the cosmological parameters are free to vary and an evolution of the correlation parameters is allowed.
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