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Table 2.

Spatial and kinematical properties of the samples, roughly ordered from younger to older (according to σu), from left to right, excluding the data from the Besançon Galactic model.

Intrinsic N-type Extrinsic Giant Tc-poor Tc-rich 5.4–2.5 1.9–1.6 1.6–1.3 1.3–1.15 1.15–1 M
S C Sa M M M 0.15–1 2–3 3–5 5–7 7–10 (Gyr)

Abia Famaey This work Besançon Galactic Model
σu (km/s) 27.4 27.7 33.1 31.8 ± 1.6 38.8 ± 0.5 46.3 ± 0.7 12.7 24.4 30.4 36.9 42.7
σv (km/s) 18.2 19.0 24.8 17.6 ± 0.8 19.7 ± 0.2 29.4 ± 1.3 7.2 13.9 17.2 21.0 24.3
σw (km/s) 15.2 12.6 16.3 16.3 ± 0.8 18.6 ± 0.4 12.3 ± 0.3 5.9 11.3 14.0 17.0 19.8
HZ (pc) 150 200 260 196 190 190
N 50 144 85b 3417 21 18

Notes. The quantities σu, σv and σw are the standard deviations of velocities in the heliocentric Galactic coordinate system; HZ is the Galactic scale height; and N is the number of stars in the sample. Predictions from the Besançon Galactic model are shown for comparison (as a function of age and main-sequence mass) for the thin disc (−0.1 ≤ [Fe/H] ≤ 0), from Robin (2021). The relation between solar-metallicity main-sequence lifetime τMS and mass M is derived from the simple relation τMS = 109 (M/M)−2.5 Gyr. See text for more detailed estimates involving low-metallicity AGB stars. a No correction has been applied to use the binary’s centre-of-mass velocity, instead of the average velocity. b Excluding star CD –54°9245, which behaves like an outlier.

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