Open Access
Table A.1.
Summary table of the parameters used to generate the CSP library.
| Parameters | Description | Prior PDF | |||
|---|---|---|---|---|---|
Secular SFH: ![]() |
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| tform, lb | |||||
| ≡t0 − tform | Time elapsed since the beginning of the SFH | Log-uniform between 5 ⋅ 108 and 2 ⋅ 1010 yr | |||
| τ | Time scale/peak | From log-uniform of τ/tform, lb between 1/20 and 2 | |||
| Secular Chemical Enrichment History: | |||||
![]() |
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| ⟨Z* fm − w⟩ | Formed-mass-weighted metallicity (non-generative, constraint for generative pars.) | tanh distribution of P(log⟨Z* fm − w⟩): P(1/50 Z⊙) = 0, P(0.1 Z⊙) = 0.9, P(3.8 Z⊙) = 1, ⟨Z* fm − w⟩ < 3.8 Z⊙ | |||
| α | Swiftness of chemical enrichment | 0.25 ≤ α ≤ 19, from a uniform distribution in ![]() |
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| Z* 0 | Initial metallicity | Log-uniform between log(Zmin/Z⊙)≡log(1/50) and min(log Z0 max/Z⊙ ≡ log(0.05),⟨Z* fm − w⟩) | |||
| Z* final | Final metallicity | Derived from Zmin, α, and ⟨Z* fm − w⟩, with the constraint Z* final ≤ 4Z* ⊙ | |||
| Bursts | |||||
| Nburst | Number of bursts | 1/3 of models without bursts; for the remaining 2/3: Nburst ≤ 6, P(Nburst)∝e−Nburst | |||
| tburst, i | Age of the ith burst (instantaneous) | Log-uniform distribution between 105 yr and the tform of the secular component | |||
| Z* burst, i | Metallicity of the ith burst | Gaussian distribution in log-Z, with mean equal to the metallicity value of the secular component at t = tburst, i and width σZ* burst = 0.2 dex | |||
| ℳburst, i | Mass fraction formed in the ith burst relative to the mass formed in secular mode | Log-uniform distribution between 10−3 and 2. More restrictive upper limits applied for tburst, i < 108 yr | |||
| Dust attenuation (Charlot & Fall 2000) | |||||
| τV | Total optical depth due to diffuse ISM and birth cloud (affects stars younger than 107 yr) | P(τV)∝1 − tanh(1.5τV − 6.7), constant at low values, exponential drop to 0 between τV = 4 and τV = 6 | |||
| μ | Fraction of total optical depth in diffuse ISM | P(μ)∝1 − tanh(8μ − 6), exponential drop to 0 between μ = 0.5 and μ = 1 | |||
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