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Table 2

Effective temperatures, surface gravities, v sin i, and vrad of our sample.

ID Johnson Strömgren Geneva Spectroscopy Adopted
Teff Teff log g Teff log g St. Teff log g v sin i vrad Teff log g
(K) (K) (cgs) (K) (cgs) comp. (K) (cgs) (km s-1) (km s-1) (K) (cgs)
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13)

HD 66765 21 000 (...) (...) 19 820 4.32 20 000 4.0 100 21 20 000 4.0
HD 67621 21 500 (...) (...) 20 580 4.22 21 000 4.0 23 18 21 000 4.0
HD 109026 16 000 16 310 4.12 16 080 4.00 A [15 000, 17 000] 4.0 180* 0* 16 000 4.0
B (...) (...) 20 0
HD 121743 22 000 20 810 3.79 21 180 4.07 21 000 4.0 60 10 21 000 4.0
HD 133518 22 000 20 670 3.98 19 400 4.29 19 000 [3.5,4.0] 0 –5 19 000 4.0
HD 147932 18 000 18 260 4.74 18 060 4.04 [16 000, 18 000] [3.75, 4.0] 140* –10* 17 000 4.0
HD 156324 21 000 (...) (...) 19 580 4.38 A 22 000 4.0 60* [10, –40, 30]** 22 000 4.0
B [14 000–17 000] (...) 30* [–30, 140, –80]**
C [14 000–17 000] (...) 5 [10, 8, 0]**
HD 156424 21 000 21 340 4.20 (...) (...) 20 000 4.0 12 0 20 000 4.0

Notes. Column (1): star identification. Columns (2), (3), and (5) effective temperature of the stars determined using Johnson, Strömgren, and Geneva photometry, respectively. Columns (4) and (6): surface gravity of the stars obtained from Strömgren and Geneva photometry. Column (7): spectroscopic stellar component in the cases of a multiple spectroscopic system (P for primary, S for secondary, T for tertiary). Columns (8) to (11) effective temperature, log g, v sin i and radial velocities estimated from our data. Columns (12) and (13): adopted effective temperatures and surface gravities for the least-squares deconvolution (LSD, Sect. 4.1). “(...)”: Not determined, because of unavailable photometric measurements.

(†)

Spectroscopic multiple systems, approximate.

(*)

Approximate (large and variable spectral lines).

(**)

Radial velocities ordered in increasing HJD. Approximate values for the component A and C due to broad, variable, or faint lines.

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