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Table 1

Results of the KS test comparing distributions of ω, Ω, L, and i of the observational data and those inferred from the benchmark model simulation at t = 4 Gyr.

Q2 = 0 ω Ω L i

p(150−250 | 150−250) 0.17 0.31 0.66 0.00
p( > 250 | > 250) 0.00 0.03 0.04 0.00

P9 (#1) ω Ω L i

p(150−250 | 150−250) 0.95 0.25 0.07 0.98

P9 (#2) ω Ω L i

p(150−250 | 150−250) 0.48 0.48 0.83 1.00

Q2 = 1 ω Ω L i

p(150−250 | 150−250) 0.19 0.03 0.71 0.00
p( > 250 | > 250) 0.02 0.00 0.01 0.00

Q2 = 2 ω Ω L i

p(150−250 | 150−250) 0.25 0.01 0.95 0.00
p( > 250 | > 250) 0.01 0.01 0.01 0.02

Q2 = 4 ω Ω L i

p(150−250 | 150−250) 0.35 0.00 0.66 0.00
p( > 250 | > 250) 0.03 0.00 0.04 0.49

Q2 = 6 ω Ω L i

p(150−250 | 150−250) 0.26 0.01 0.80 0.07
p( > 250 | > 250) 0.00 0.00 0.01 0.89

Notes. The KS test was also carried out for the P9 simulation. Each simulation starts with 400 particles; p(ξ | ζ) is the probability p-value, where ξ are the observational data in a quoted a-range, and ζ are the simulated data in a quoted a-range, e.g. p(150−250 | 150−250) is the p-value comparing the observational and simulated data in range 150 <a< 250 au. The p-values larger than 0.5 are highlighted in boldface. There was only one particle with a> 250 au left at the end of the P9 simulation, therefore p( > 250 | > 250) is not reported in this case; [Q2] = 10-27 s-2.

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