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Table 1

Photospheric physical parameters obtained through the fittings with ZPEKTR models to the observed Be’s median spectra available at the BeSOS database, within the range 4450–4500 Å.

Target Teff (K) log g(cgs) v sin i (km s−1) Teff (K) log g(cgs) v sin i (km s−1)
PNRC PNRC PNRC apparent apparent apparent
HD 10144 (α Eri) 18 200 ± 550 3.5 ± 0.2 246 ± 9 15 500 ± 450 2.9 ± 0.1 228 ± 10
HD 33328 (λ Eri) 25 200 ± 750 4.2 ± 0.2 311 ± 10 21 500 ± 650 3.5 ± 0.1 280 ± 10
HD 35411 (η Ori) 29 500 ± 1150 4.2 ± 0.2 292 ± 10 25 500 ± 1050 3.6 ± 0.1 280 ± 10
HD 37795 (α Col) 13 900 ± 400 3.7 ± 0.1 207 ± 9 12 500 ± 375 3.1 ± 0.1 170 ± 8
HD 50013 (κ CMa) 27 300 ± 800 3.9 ± 0.1 238 ± 10 24 500 ± 750 3.2 ± 0.1 220 ± 10
HD 56014 (27 CMa) 21 200 ± 650 3.7 ± 0.1 255 ± 10 18 000 ± 540 3.5 ± 0.1 170 ± 10
HD 57150 (NV Pup) 23 000 ± 700 3.7 ± 0.1 212 ± 9 22 000 ± 650 3.5 ± 0.1 190 ± 12
HD 58715 (β CMi) 12 000 ± 350 3.7 ± 0.1 272 ± 20 11 000± 350 3.4 ± 0.1 210 ± 8
HD 63462 (o Pup) 27 500 ± 1100 3.2 ± 0.1 326 ± 10 24 000 ± 960 2.9 ± 0.1 300 ± 10
HD 68980 (MX Pup) 23 600 ± 750 3.3 ± 0.1 121 ± 8 23 500 ± 750 3.1 ± 0.1 110 ± 8
HD 75311 (V344 Car) 20 000 ± 600 4.1 ± 0.1 245 ± 15 19 000 ± 580 3.9 ± 0.1 268 ± 12
HD 83953 (I Hya) 16 600 ± 500 3.9 ± 0.1 296 ± 15 15 000 ± 500 2.6 ± 0.1 260 ± 10
HD 89080 (ω Car) 12 500 ± 400 3.7 ± 0.1 271 ± 15 11 500 ± 400 3.4 ± 0.2 240 ± 12
HD 91465 (p Car) 19 500 ± 550 3.7 ± 0.1 298 ± 11 17 000 ± 510 3.2 ± 0.1 266 ± 10
HD 93563 15200 ± 500 3.6 ± 0.1 269 ± 15 13 500 ± 450 2.5 ± 0.1 218 ± 10
HD 103192 (β Hya) 10 800 ± 350 2.4 ± 0.1 101 ± 10 9000 ± 350 1.5 ± 0.3 95 ± 10
HD 120324 (μ Cen) 23 700 ± 800 4.0 ± 0.1 129 ± 10 22 500 ± 800 3.7 ± 0.1 125 ± 10
HD 124771 (ϵ Aps) 18 000 ± 600 4.0 ± 0.1 163 ± 10 17 000 ± 500 3.5 ± 0.1 150 ± 10
HD 127972 (η Cen) 21 700 ± 700 4.0 ± 0.1 246 ± 11 19 500 ± 700 3.5 ± 0.1 240 ± 12
HD 131492 (θ Cir) 19 500 ± 700 3.7 ± 0.2 123 ± 13 17 500 ± 700 3.6 ± 0.2 100 ± 13
HD 135734 (μ Lup) 12 000 ± 400 3.5 ± 0.1 127 ± 10 11 000± 400 2.5 ± 0.1 100 ± 10
HD 138769 (d Lup) 18 500 ± 600 3.9 ± 0.1 87 ± 5 16 500 ± 600 3.7 ± 0.1 80 ± 5
HD 143275 (δ Sco) 27 000 ± 950 2.9 ± 0.1 195 ± 13 25 500 ± 900 2.4 ± 0.1 175 ± 12
HD 157246 (γ Ara) 24 000 ± 800 4.3 ± 0.2 250 ± 12 21 500 ± 700 3.6 ± 0.1 230 ± 5
HD 158427 (α Ara) 21 500 ± 700 4.5 ± 0.2 308 ± 15 18 000 ± 600 3.8 ± 0.2 285 ± 15
HD 205637 (ε Cap) 22 000 ± 700 4.8 ± 0.2 240 ± 10 19 000 ± 700 4.2 ± 0.1 230 ± 10
HD 209014 (η PsA) 13 000 ± 500 3.8 ± 0.1 331 ± 10 11 500 ± 500 3.0 ± 0.1 320 ± 10
HD 212076 (31 Peg) 17 950 ± 600 3.5 ± 0.1 104 ± 12 18 000 ± 600 3.5 ± 0.1 98 ± 12
HD 212571 (π Aqr) 26 000 ± 900 3.8 ± 0.1 226 ± 5 24 500 ± 800 3.4 ± 0.1 215 ± 5
HD 217891 (β Psc) 16 000 ± 500 3.2 ± 0.1 105 ± 3 15 000 ± 500 3.0 ± 0.1 95 ± 3
HD 219688 (ψ2 Aqr) 16 300 ± 500 4.1 ± 0.1 338 ± 10 14 500 ± 500 3.9 ± 0.1 290 ± 10

Notes. In these analyses, we assumed the classical von Zeipel model with β = 0.25. Teff (PNRC), log g (PNRC), and v sin i (PNRC) are, respectively, the surface temperature, gravity, and the projected rotation velocity of the PNRC, which are the parameters these stars would present in the absence of geometrical deformation and (T, log g) colatitudinal dependence. Apparent parameters are those calculated with classical model atmospheres.

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