Table 2
Summary of regression statistics for all triple orbital configurations, for regression equations aio ∕a2, aoi ∕a2 = C + b1μ1 + b2μ2 + b3e1 + b4e2 + b5i2 + b6Ω2 + b7ω2.
Orbit | Crit. | Higha | Motionsb | Crit. semi-major axis ratio | Regression coefficients | Integrations | Model fit | |||||||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
type | ratio | incl. | Star 3 | Planet | Min | Mean | σ | Max | C | a | μ1 | μ2 | e1 | e2 | i2 | Ω2 | ω2 | No. | Bounds | Rate | R2 | F | SE | MAPE |
found | (%) | (%) | ||||||||||||||||||||||
P1 | aio ∕a2 | P | P | 0.131 | 0.383 | 0.147 | 0.892 | 0.439 | 0.000 | −0.005 | −0.020 | −0.004 | −0.114 | 0.000 | −0.001 | −0.001 | 5 413 | 1 782 | 33 | 0.132 | 34 | 0.093 | 19 | |
R | 0.113 | 0.519 | 0.108 | 0.828 | 0.572 | 0.000 | 0.009 | −0.043 | −0.010 | −0.468 | 0.000 | 0.000 | 0.000 | 5 343 | 976 | 18 | 0.670 | 241 | 0.062 | 10 | ||||
R | P | 0.110 | 0.385 | 0.077 | 0.897 | 0.463 | 0.000 | 0.192 | −0.037 | −0.021 | −0.187 | −0.001 | 0.000 | 0.000 | 2 122 | 569 | 27 | 0.547 | 285 | 0.358 | 9 | |||
R | 0.112 | 0.537 | 0.132 | 0.857 | 0.656 | 0.000 | −0.056 | −0.022 | 0.005 | −0.510 | 0.000 | 0.000 | 0.000 | 2 685 | 539 | 20 | 0.710 | 162 | 0.071 | 12 | ||||
NK | P | P | 0.049 | 0.484 | 0.099 | 0.837 | 0.545 | 0.000 | −0.044 | −0.018 | 0.000 | 0.000 | −0.001 | 0.000 | 0.000 | 342 | 256 | 75 | 0.024 | 2 | 0.099 | 18 | ||
K | P | 0.288 | 0.495 | 0.100 | 0.748 | 0.303 | 0.001 | −0.170 | 0.017 | 0.000 | 0.000 | 0.002 | 0.000 | 0.000 | 319 | 47 | 15 | 0.177 | 2 | 0.095 | 19 | |||
NK | R | P | 0.423 | 0.666 | 0.078 | 0.853 | 0.685 | −0.001 | 0.066 | 0.029 | 0.000 | 0.000 | −0.001 | 0.000 | 0.000 | 273 | 178 | 65 | 0.202 | 4 | 0.024 | 13 | ||
K | P | 0.105 | 0.531 | 0.096 | 0.818 | 0.738 | 0.000 | −0.038 | −0.083 | 0.000 | 0.000 | −0.001 | 0.000 | 0.000 | 207 | 102 | 49 | 0.194 | 6 | 0.088 | 12 | |||
P2 | aoi ∕a2 | P | P | 1.253 | 2.936 | 1.449 | 5.197 | 2.376 | −0.003 | 0.053 | 0.044 | 0.090 | 1.996 | 0.000 | −0.001 | −0.002 | 5 413 | 5 133 | 95 | 0.829 | 3 097 | 0.248 | 6 | |
R | 1.184 | 1.976 | 0.507 | 4.916 | 1.482 | −0.004 | 0.131 | −0.008 | −0.036 | 1.727 | 0.001 | 0.001 | 0.001 | 5 343 | 5 082 | 95 | 0.865 | 3 910 | 0.198 | 6 | ||||
R | P | 0.924 | 2.773 | 0.891 | 5.384 | 2.089 | −0.004 | 0.809 | 0.114 | 0.015 | 1.298 | −0.001 | 0.000 | 0.000 | 2 122 | 1 895 | 89 | 0.271 | 26 | 0.126 | 31 | |||
R | 0.591 | 1.960 | 0.571 | 4.957 | 1.708 | −0.005 | 0.182 | 0.023 | 0.018 | 1.693 | −0.001 | 0.000 | 0.000 | 2 685 | 2 455 | 91 | 0.773 | 1 039 | 0.269 | 8 | ||||
NK | P | P | 1.755 | 1.941 | 0.051 | 2.242 | 1.920 | −0.002 | 0.048 | 0.016 | 0.000 | 0.000 | 0.002 | 0.000 | 0.000 | 342 | 341 | 100 | 0.269 | 30 | 0.044 | 4 | ||
K | P | 1.759 | 1.933 | 0.176 | 2.532 | 2.345 | −0.004 | 0.066 | 0.043 | 0.000 | 0.000 | −0.003 | 0.000 | 0.000 | 319 | 319 | 100 | 0.589 | 117 | 0.115 | 3 | |||
NK | R | P | 1.095 | 1.335 | 0.127 | 1.820 | 1.288 | −0.002 | 0.085 | −0.004 | 0.000 | 0.000 | 0.007 | 0.000 | 0.000 | 273 | 273 | 100 | 0.555 | 83 | 0.085 | 4 | ||
K | P | 1.363 | 1.753 | 0.195 | 2.510 | 1.356 | −0.003 | 0.033 | −0.016 | 0.000 | 0.000 | 0.008 | 0.000 | 0.000 | 207 | 204 | 99 | 0.574 | 64 | 0.129 | 5 | |||
S1 | aio ∕a1 | P | P | 0.015 | 0.180 | 0.049 | 0.760 | 0.390 | 0.000 | −0.746 | 0.005 | −0.398 | −0.006 | 0.000 | 0.000 | 0.000 | 1 532 | 819 | 54 | 0.583 | 142 | 0.081 | 35 | |
R | 0.015 | 0.185 | 0.122 | 0.771 | 0.392 | 0.000 | −0.667 | 0.003 | −0.381 | 0.002 | 0.000 | 0.000 | 0.000 | 1 480 | 785 | 53 | 0.567 | 131 | 0.081 | 37 | ||||
R | P | 0.015 | 0.197 | 0.059 | 0.772 | 0.277 | 0.000 | −0.387 | −0.005 | −0.125 | −0.005 | 0.000 | 0.000 | 0.000 | 1 586 | 957 | 60 | 0.126 | 17 | 0.139 | 67 | |||
R | 0.028 | 0.196 | 0.157 | 0.772 | 0.423 | 0.000 | −0.451 | −0.006 | −0.056 | −0.048 | 0.001 | 0.000 | 0.000 | 1 455 | 791 | 54 | 0.176 | 20 | 0.143 | 74 | ||||
S3 | aio ∕a2 | P | P | 0.009 | 0.289 | 0.098 | 0.893 | 0.393 | 0.000 | −0.075 | 0.037 | −0.020 | −0.604 | 0.000 | 0.000 | 0.000 | 1 604 | 1 599 | 100 | 0.712 | 481 | 0.084 | 25 | |
R | 0.010 | 0.361 | 0.158 | 0.920 | 0.444 | 0.001 | 0.001 | 0.113 | −0.011 | −0.580 | 0.000 | 0.000 | 0.000 | 1 562 | 1 501 | 96 | 0.790 | 705 | 0.071 | 17 | ||||
R | P | 0.007 | 0.287 | 0.096 | 0.853 | 0.391 | 0.002 | −0.071 | 0.033 | −0.001 | −0.597 | 0.000 | 0.000 | 0.000 | 1 596 | 1 591 | 100 | 0.727 | 522 | 0.077 | 23 | |||
R | 0.009 | 0.360 | 0.156 | 0.908 | 0.425 | 0.000 | −0.002 | 0.114 | −0.002 | −0.580 | 0.000 | 0.000 | 0.000 | 1 537 | 1 489 | 97 | 0.790 | 688 | 0.071 | 17 | ||||
Averagec /totald | 0.473 | 0.944 | 0.237 | 1.789 | 0.921 | 0.000 | 0.183 | 0.036 | 0.050 | 0.433 | 0.001 | 0.000 | 0.000 | 45 760 | 29 683 | 65 | 0.495 | – | – | – |
Notes. The directional movements of the stability bounds for planetary orbits are generally as expected, except for retrograde inner planetary orbits, for which the bound increases instead of shrinking. This may be attributable to the small sample, since very few retrograde star/retrograde planet combinations were stable. Italics denote coefficients with signs that were not as expected. Ignoring coefficients smaller than 0.01, only four did not have the expected sign and these were all small (< |0.06|). The semi-major axis ratio a is included as an error check as the critical ratio scales with it and its coefficient should be zero. Its average absolute value of < 0.0005 therefore provides an indication of the intrinsic error of the methodology. (a) NK – non-Kozai, K – Kozai. (b) P – prograde, R – retrograde. (c) Of absolute values for regression coefficients. (d)Of integrations and bounds.
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