Table 1.
Parameter settings of the chi-squared simulations.
# | Model name | Opacity (a) | A2 | Abundance | tacc(b) | Composition | fovershoot |
---|---|---|---|---|---|---|---|
table | [Myr] | of accreted | |||||
material (c) | |||||||
[Optimized non-accreting models] | |||||||
1 | noacc | S | – | AGSS09 | – | – | variable |
2 | noacc-GS98 | S | – | GS98 | – | – | variable |
3 | noacc-noov | S | – | AGSS09 | – | – | 0 |
4 | noacc-GS98-noov | S | – | GS98 | – | – | 0 |
[Optimization with time-dependent Yacc (He-poor accretion)] | |||||||
5 | He12Myr | S | – | AGSS09 | 12 | Y | variable |
6 | He20Myr | S | – | AGSS09 | 20 | Y | variable |
[Optimization with time-dependent Zacc (pebble wave and planet formation)] | |||||||
7 | MZvar | S | – | AGSS09 | 10 | Z | variable |
8 | MZvar-noov | S | – | AGSS09 | 10 | Z | 0 |
[Optimization with opacity enhancement and homogeneous Zacc and Yacc] | |||||||
9 | K2 | K2 | [0, 0.22] | AGSS09 | 10 | H | variable |
10 | K23 | K23 | [0, 0.22] | AGSS09 | 10 | H | variable |
11 | K23′ | ![]() |
0.10 | AGSS09 | 10 | H | variable |
12 | K2′ | K2 | 0.12/0.15/0.18 | AGSS09 | 3/5/10 | H | 0/0.01/0.025 |
[Optimization with opacity enhancement and time-dependent Zacc] | |||||||
13 | K2-MZvar | K2 | 0.12/0.15/0.18 | AGSS09 | 10 | Z | variable |
14 | K23-MZvar | K23 | 0.12/0.15/0.18 | AGSS09 | 10 | Z | variable |
15 | K2-MZ | K2 | 0.12 | AGSS09 | 5 | Z′ | 0.01 |
16 | K2-MZ1′/MZ8′ | K2 | 0.12/0.15/0.18 | AGSS09 | 3/5/10 | Z′ | 0/0.01/0.025 |
Notes.
S: Standard (i.e., no modification to the opacity). K2: Enhanced opacity (κ) using Gaussian functions with A1 = A3 = 0 and A2 fixed to a value between 0 and 0.22 (see Sect. 3.1.5). K23: Same as K2 but A3 varies in the simplex method. : A2 = 0.10 (fixed) and A3 is fixed to either 0.05 or −0.05.
Accretion timescale (see Sect. 3.1.2).
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