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Table 2.

Means and standard deviations for mass ratios, orbital periods, radii, inclination angles, and phases of the triple for each light fraction.

fAa/fTotal 0.92–0.96 0.83–0.87 Free Units

Mean σ Mean σ Mean σ
M Aa M Ab 1 + M Ab 2 $ \frac{M_{\mathrm{Aa}}}{M_{\mathrm{Ab1}}+M_{\mathrm{Ab2}}} $ 3.60899 0.009644 3.616071 0.011244 3.609757 0.011643
M Ab 1 M Ab 2 $ \frac{M_{\mathrm{Ab1}}}{M_{\mathrm{Ab2}}} $ 1.113493 0.001189 1.113638 0.001121 1.113805 0.001068
a Aab a Ab 1 Ab 2 $ \frac{a_{\mathrm{Aab}}}{a_{\mathrm{Ab1Ab2}}} $ 21.8186 0.011018 21.819058 0.011902 21.814642 0.01216
PAab 94.294862 0.000079 94.29485 0.000086 94.294881 0.000088 Days
PAb1Ab2 1.522248 0.000001 1.522248 0.000001 1.522248 0.000001 Days
RAa 1.651985 0.008722 1.62128 0.009831 1.609895 0.018195 R
RAb1 0.421674 0.002214 0.432398 0.002659 0.432924 0.003544 R
RAb2 0.378438 0.002011 0.38805 0.002384 0.388529 0.003222 R
iAaAb 0.408563 0.006962 0.362485 0.007541 0.35407 0.017894 °
iAb1Ab2 0.405657 0.051257 0.42117 0.059913 0.424795 0.063631 °
ϕAab 4.199443 0.00002 4.199436 0.00002 4.199438 0.00002 Radians
ϕAb1b2 1.532349 0.001102 1.532399 0.000987 1.532342 0.001016 Radians

Notes. We define our inclination angles with 0° being edge-on. The merit values of the converged state of all three simulations vary between 650–630, 645–625, and 645–625 for the 0.92–0.96, 0.83–0.87, and free light-fraction simulations, respectively. This implies a small statistical benefit when considering light fractions below 0.92, but no statistical benefit to the fit when considering light fractions below 0.83.

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