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Table 3.

Characteristics of the three ejection events analyzed in this paper.

Event N Weighted Cluster tmin αmin δmin rtα rtδ rαδ
motion (ka) (deg) (deg)
Bajamar 5 No Kept 1611 12 313.575 0.011 44.099 0.020 −0.54 −0.69 +0.45
Yes Kept 1611 11 313.577 0.011 44.095 0.015 −0.75 −0.72 +0.69
No Subtracted 313.107 0.014 44.442 0.019 −0.74 −0.62 +0.53
Yes Subtracted 313.109 0.014 44.440 0.014 −0.86 −0.65 +0.69

Toronto 2 No Kept 1503 51 313.403 0.045 44.045 0.051 −0.31 −0.95 +0.41
Yes Kept 1496 44 313.434 0.039 44.062 0.045 −0.28 −0.96 +0.39
No Subtracted 312.971 0.053 44.367 0.042 −0.59 −0.92 +0.66
Yes Subtracted 313.005 0.045 44.382 0.037 −0.57 −0.94 +0.65

HD 201 795 2 No Kept 1923 62 313.654 0.047 43.947 0.070 −0.47 −0.93 +0.18
Yes Kept 1905 37 313.641 0.039 43.985 0.039 −0.59 −0.89 +0.22
No Subtracted 313.076 0.061 44.346 0.060 −0.72 −0.91 +0.43
Yes Subtracted 313.070 0.048 44.381 0.036 −0.76 −0.85 +0.36

Notes. The columns give (a) the number of systems involved in each event; (b) whether the results are weighted or not by the Gaussian factors, (c) whether the cluster motion has been subtracted or not; and (d) the flight times, event positions, and their correlations.

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