Table 1
Initial parameters of the model galaxies.
| Model | T[Gyr] | Init.M•[M9] | Mdyn[M9] | Re[kpc] | Rb[kpc] | ΔM•[M9] | Comment |
|
|
|||||||
| 1 | 8 | 1.5 | 400 | 4 | 0.15 | 0.06 | OB-low, ϵ = 0.42 |
| 2 | 8 | 5 | 770 | 7 | 0.4 | 0.17 | OB-low, ϵ = 0.2 |
| 3 | 8 | 10 | 1550 | 18 | 0.8 | 0.38 | OB-low, ϵ = 0.1 |
| 4 | 8 | 10 | 1550 | 18 | 0.8 | 0.7 | OB-low, ϵ = 0.057 |
| 5 | 8 | 15 | 1750 | 25 | 1.3 | 4 | OB-medium, ϵ = 0.1 |
| 6 | 8 | 20 | 1750 | 25 | 1.8 | 6 | OB-high, ϵ = 0.2 |
| 7 | 8 | 20 | 1750 | 25 | 1.8 | 13 | OB-high, ϵ = 0.1 |
| 8 | 8 | 40 | 2000 | 68 | 3.8 | 40 | OB-medium, ϵ = 0.01 |
| 9 | 6.7 | 40 | 2000 | 68 | 3.8 | 120 | OB-high, ϵ = 0.01 |
Notes. List of parameters selected for our models/N-body computations. OB stands for observation-based models (Sect. 2.2). Slope values γ = 0.2, α = 4.25, and n = 4 (Eq. (6)) are used for all models. The huge initial SMBH masses in excess of 1010 M⊙ are motivated at the end of Sect. 2.2 and in Sect. 2.3. While dynamical masses, Mdyn, and effective radii, Re, of our model galaxies are constrained by representative galaxies, the break-radius, Rb, is taken from the scaling relation in Rusli et al. (2013). SMBH masses during the N-body computations are linearly increased up to ΔM• over the typical galaxy cluster lifetime of T ≈ 8 Gyr. The ΔM• values are selected to equally cover (in log-space) the whole parameter range of SMBH growth rates, which are specified in Sect. 2. Model 9 is computed from z = 1 until z = 0.1.
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