Table B.2
Summary table for all the background cosmology and models available in ICAROGW. The same mass models are also available for NSBH binaries. NSBH models also include three extra parameters: that are the minimum and maximum mass of the NS and the smoothing window for the lower end of the NS mass spectrum, respectively. More details on the models can be found in Sect. B.2.
Model name | Population parameters | |
---|---|---|
Symbol | Description | |
Power law | −α | Power law index primary mass |
β | Power law index secondary mass | |
mmin | Minimum source mass [M⊙] | |
mmax | Maximum source mass [M⊙] | |
Power law + peak | −α | Power law index primary mass |
β | Power law index secondary mass | |
mmin | Minimum source mass [M⊙] | |
mmax | Maximum source mass [M⊙] | |
δm | Smoothing parameter [M⊙] Eq. (B.12) | |
μ𝑔 | Peak of the Gaussian [M⊙] | |
σ𝑔 | s.t.d of the Gaussian [M⊙] | |
λpeak | Fraction of events in Gaussian ∈ [0, 1] | |
Broken power law | −α1 | First power law index primary mass |
−α2 | Second power law index primary mass | |
β | Power law index secondary mass | |
mmin | Minimum source mass [M⊙] | |
mmax | Maximum source mass [M⊙] | |
δm | Smoothing parameter [M⊙] Eq. (B.12) | |
b | Defines mbreak = b(mmax − mmin) | |
Multi-peak | −α | Power law index primary mass |
β | Power law index secondary mass | |
mmin | Minimum source mass [M⊙] | |
mmax | Maximum source mass [M⊙] | |
δm | Smoothing parameter [M⊙] Eq. (B.12) | |
μ𝑔,low | Peak lower mass Gaussian [M⊙] | |
σ𝑔,low | s.t.d. of the lower mass Gaussian in [M⊙] | |
μ𝑔,high | Peak higher mass Gaussian [M⊙] | |
σ𝑔,high | s.t.d higher mass Gaussian in [M⊙] | |
λg | Events in Gaussians ∈ [0, 1] | |
λg, low | Events in lower Gaussian ∈ [0, 1] |
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