Table 1
Initial parameters of different runs.
Model | Σ1(R = 0) | h 2 | σR1(R = 0) | σR2(R = 0) |
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α | β | Qmax(α,β) | Q1(R = R∗) | Qeff(R = R∗) | |||||
M⊙ pc-2 | kpc | km s-1 | km s-1 | |||||||||||||
|
||||||||||||||||
A† | 750 | 3 | 60 | 35 | 0.5 | 0.5 | 0.5 | 0.34 | 1.8 | 1.44 | 0.8 | |||||
B† | 750 | 3 | 100 | 35 | 0.5 | 0.5 | 0.5 | 0.12 | 2.2 | 2.2 | 1.0 | |||||
|
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C | 750 | 3 | 60 | 35 | 0.5 | 0.5 | 0.5 | 0.34 | 1.8 | 1.44 | 0.8 | |||||
D | 750 | 3 | 100 | 35 | 0.5 | 0.5 | 0.5 | 0.12 | 2.2 | 2.2 | 1.0 | |||||
E | 400 | 3 | 100 | 35 | 0.5 | 0.5 | 0.5 | 0.12 | 2.2 | 3.96 | 1.8 | |||||
G | 400 | 3 | 60 | 35 | 0.5 | 0.5 | 0.5 | 0.34 | 1.8 | 2.8 | 1.5 | |||||
|
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I01 | 1050 | 3 | 50 | 50 | 0.5 | 0.5 | 0.1 | 1 | 1.08 | 1.0 | 1.0 | |||||
I02 | 970 | 3 | 50 | 50 | 0.5 | 0.5 | 0.2 | 1 | 1.2 | 1.2 | 1.0 | |||||
I03 | 895 | 3 | 50 | 50 | 0.5 | 0.5 | 0.3 | 1 | 1.3 | 1.3 | 1.0 | |||||
I04 | 830 | 3 | 50 | 50 | 0.5 | 0.5 | 0.4 | 1 | 1.4 | 1.4 | 1.0 | |||||
I05 | 775 | 3 | 50 | 50 | 0.5 | 0.5 | 0.5 | 1 | 1.5 | 1.5 | 1.0 | |||||
I07 | 660 | 3 | 50 | 50 | 0.5 | 0.5 | 0.7 | 1 | 1.7 | 1.7 | 1.0 | |||||
I10 | 525 | 3 | 50 | 50 | 0.5 | 0.5 | 1 | 1 | 2.0 | 2.7 | 1.4 | |||||
|
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Kb | 750 | 2 | 90 | 30 | 0.7 | 0.4 | 0.5 | 0.12 | 1.48 | 1.48 | 1.0 | |||||
Kc | 750 | 5 | 90 | 30 | 0.6 | 0.2 | 0.5 | 0.1 | 1.51 | 1.51 | 1.0 |
Notes. Models without counterrotation are marked by † (δ = 1). Here Σ1(R = 0) is the central value of the surface density of the primary component, h2 is the exponential scale length of the density distribution of the second component (for the first component, h1 = 3 kpc), σR1(R = 0) and σR2(R = 0) are the central values of the velocity dispersion for each component, Q1(R = R∗) is the minimum value of the one-component stability parameter of the host component, and Qeff(R = R∗) is the effective two-component stability parameter according to Eq. (7) evaluated at R∗. Initial values of the velocity dispersion ratio for the two components are constant with radius for all models. The definitions of the density ratio α and of the temperature ratio β are given in the text; also these parameters are generally constant with radius, except for models Kb and Kc, for which the values listed here are taken at R = R∗, that is, the location where Q1 has its minimum. Model I10 considers the case of exactly equal but counterrotating disks, which is unlikely to occur in real systems.
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