Table 2

Results for the disc simulations with the initial conditions listed in Table 1 after 30 kyr of evolution.

Run M (M) Mdisc (M) ΔMdisc (Mj) t (kyr) q Rdisc (AU) afrag (AU)
01 0.205 0.075 36.6 22.1 0.37 75 49
02 0.205 0.077 38.9 23.3 0.38 72 35
03

04 0.205 0.104 56.2 25.9 0.51 92 54
05 0.206 0.105 57.2 27.6 0.51 137 55
06 0.207 0.106 58.1 28.0 0.51 169 32

07 0.204 0.124 68.7 26.7 0.61 144 46
08 0.205 0.126 70.8 27.6 0.62 128 30
09 0.207 0.128 72.2 28.8 0.62 190 54

10 0.305 0.094 46.9 18.5 0.31 96 40
11 0.305 0.097 50.2 19.6 0.32 68 32
12

13 0.305 0.122 63.0 19.2 0.40 89 59
14 0.305 0.125 66.3 20.2 0.41 89 28
15

16 0.304 0.146 77.8 20.0 0.48 131 55
17 0.305 0.150 81.7 21.0 0.49 126 60
18 0.307 0.155 86.7 22.7 0.50 159 84

19
20
21

22 0.405 0.144 76.2 17.3 0.36 105 57
23 0.405 0.140 72.1 16.4 0.35 91 37
24

25 0.405 0.165 86.1 16.5 0.41 123 47
26 0.405 0.171 91.6 17.6 0.42 130 43
27 0.407 0.176 97.4 19.0 0.43 164 116

Notes. M and Mdisc are respectively the masses of the star and disc when the disc fragments. t is the time at which fragmentation occurs, q is the disc-to-star mass ratio at fragmentation and Rdisc is the radius of the disc. afrag is the distance of the fragment from the host star. Some discs did not fragment as noted by dashes in the corresponding rows.

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