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Table 1.

Properties of the clusters considered in this study.

Cluster d tCMD tDT σp σv R50 nstars ndiv neva neva, 70 ϕeva σeva
[pc] [Myr] [Myr] [Myr] [pc] [km s−1] [pc]
α Sco 1 148 (b) 0.31 0.07 7.8 57 21 7 2 0.93 1.12
α Sco 2 148 (b) 0.62 0.10 6.8 78 33 6 2 0.89 1.16
β Sco 153 (a) (b) 0.53 0.12 4.7 61 14 16 4 0.88 0.74
δ Sco 142 (a) (b) 0.42 0.09 4.7 131 13 52 16 0.89 0.24
ν Sco 139 (a) (b) 0.39 0.13 2.0 57 22 6 2 0.91 1.14
π Sco 123 (b) 0.26 0.13 15.7 88 17 27 8 0.88 0.37
σ Sco 152 (b) 0.63 0.14 9.8 104 25 27 6 0.88 0.49
ρ Oph 139 (a) (b) 0.52 0.10 3.3 94 37 10 3 0.88 0.74
β Pic 40 (a) (c) 0.13 0.29 24.3 26 0 13 4 0.87 0.60
Tuc-Hor 47 (a) (d) 0.03 0.40 17.1 21 2 8 3 0.87 0.61

Notes. Columns indicate (1) the cluster name, (2) the distance to the cluster, (3) the CMD age from the PARSEC isochrones used in this work, (4) the dynamical traceback age, (5) the corrected evaporation age determined in this work, (6–7) the observational error in positions and velocities, (8) the core radius, (9) the number of stars used to obtain the CMD and dynamical traceback ages and the starting sample for the evaporation ages, (10) the number of divergent stars, (11) the number of evaporated stars, (12) the number of stars used to compute the evaporation age, and (13–14) the correction factor and the uncertainty of the evaporation age (see Appendix B).

References. (a) Miret-Roig et al. (2024); (b) Miret-Roig et al. (2022); (c) Miret-Roig et al. (2020); (d) Galli et al. (2023).

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