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Table 3:

Established spectral type, literature photometry, estimated distance, radial and projected rotational velocity, observed H$\alpha $ and forbidden line emission.
    $T_{\rm eff}$ B V E(B-V) AV $d_{\rm phot}$ $v ~{\rm sin}(i)$ vr    
Star Sp.Type [K] [mag] [mag] [mag] [mag] [kpc] [km s-1] [km s-1] H$\alpha $ F.L.
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12)
Confirmed Herbig Ae/Be and T Tauri stars
Hen 3-1121S B0Ve 30 000 11.6 $\pm$ 0.1 11.1 $\pm$ 0.1 0.85 $\pm$ 0.14 2.7 $\pm$ 0.5 3.1 $^{\rm +1.0}_{-0.8}$ 240 $\pm$ 20 -28 $\pm$ 5 I [O I]
Hen 3-1121N B0.5Ve 27 500 ... 13.0 $\pm$ 0.4 1.3 $\pm$ $0.7^\star$ 4.1 $\pm$ 2.3 3.2 $^{\rm +6.3}_{-2.1}$ 245 $\pm$ 20 -58 $\pm$ 5 I [O I] [N II]
MWC 878 B1Ve 25 400 11.2 $\pm$ 0.1 10.8 $\pm$ 0.1 0.74 $\pm$ 0.15 2.3 $\pm$ 0.5 2.1 $^{\rm +0.9}_{-0.6}$ ... -11 $\pm$ 3* I [O I] [N II]
WRAY 15-1435 B1Ve 25 400 12.8 $\pm$ 0.5 12.0 $\pm$ 0.5 1.0 $\pm$ 0.7 3.2 $\pm$ 2.2 2.6 $^{\rm +5}_{-1.7}$ 230 $\pm$ 20 -30 $\pm$ 10 I [O I]
MWC 953 B2Ve 22 000 12.0 $\pm$ 0.2 10.9 $\pm$ 0.1 1.3 $\pm$ 0.2 4.0 $\pm$ 0.7 0.8 $^{\rm +0.5}_{-0.3}$ <7 23 $\pm$ 2 II [O I]
HD 313571 B3Ve 18 700 10.3 $\pm$ 0.1 9.9 $\pm$ 0.1 0.57 $\pm$ 0.15 1.8 $\pm$ 0.5 0.9 $^{\rm +0.4}_{-0.3}$ 380 $\pm$ 20 -50 $\pm$ 20 I [O I]
Hen 3-823 B3Ve 18 700 10.5 $\pm$ 0.1 10.4 $\pm$ 0.1 0.33 $\pm$ 0.15 1.0 $\pm$ 0.5 1.6 $^{\rm +0.8}_{-0.5}$ 310 $\pm$ 20 -10 $\pm$ 10 II [O I]
MWC 593 B4Ve 17 000 10.5 $\pm$ 0.1 10.0 $\pm$ 0.1 0.65 $\pm$ 0.15 2.1 $\pm$ 0.5 0.7 $^{\rm +0.2}_{-0.2}$ 330 $\pm$ 30 -20 $\pm$ 10 I [O I]
Hen 2-80 B6Ve 14 000 14.0 $\pm$ 0.1 13.2 $\pm$ 0.1 0.97 $\pm$ 0.15 3.0 $\pm$ 0.5 1.6 $^{\rm +0.5}_{-0.4}$ 60 $\pm$ 10 -22 $\pm$ 3 II [O I][S II]
WRAY 15-1372 B6Ve 14 000 11.7 $\pm$ 0.1 11.1 $\pm$ 0.1 0.80 $\pm$ 0.15 2.5 $\pm$ 0.5 0.8 $^{\rm +0.2}_{-0.17}$ 280 $\pm$ 20 -30 $\pm$ 10 II ...
Th 17-35 B8Ve 11 900 13.9 $\pm$ 0.1 13.5 $\pm$ 0.1 0.58 $\pm$ 0.15 1.8 $\pm$ 0.5 2.4 $^{\rm +0.8}_{-0.6}$ 210 $\pm$ 20 -10 $\pm$ 5 I [O I]
HD 145718 A5Ve 8200 9.3 $\pm$ 0.1 8.9 $\pm$ 0.1 0.24 $\pm$ 0.15 0.8 $\pm$ 0.5 0.17 $^{\rm +0.05}_{-0.04}$ 100 $\pm$ 10 0 $\pm$ 3 IV ...
CD-38 4380 F4Ve 6590 10.4 $\pm$ 0.1 10.0 $\pm$ 0.1 0.0 $\pm$ 0.15 0.0 $^{\rm +0.5}_{-0.0}$ 0.19 $^{\rm +0.05}_{-0.04}$ 45 $\pm$ 4 20 $\pm$ 2 I ...
Hen 3-1145 M1IVe 3720 15.3 $\pm$ 0.1 14.0 $\pm$ 0.1 -0.15 $\pm$ 0.15 0.0 $^{\rm +0.1}_{-0.0}$ 0.16 $^{\rm +0.05}_{-0.04}$ <7 -2 $\pm$ 1 I [O I]
Giant stars with emission lines that may be Herbig Ae/Be stars
HD 152291 B1IIIe 24 000 9.0 $\pm$ 0.1 9.0 $\pm$ 0.1 0.28 $\pm$ 0.15 0.9 $\pm$ 0.5 3.1 $^{\rm +1.3}_{-0.9}$ 320 $\pm$ 20 -20 $\pm$ 10 II ...
Hen 3-416 A1IIIe 9480 11.9 $\pm$ 0.2 10.8 $\pm$ 0.1 1.0 $\pm$ 0.2 3.3 $\pm$ 0.7 0.29 $^{\rm +0.12}_{-0.08}$ 30 $\pm$ 5 33 $\pm$ 4 III, IV [O I]
WRAY 15-488 F2IIIe 6870 10.3 $\pm$ 0.1  9.8 $\pm$ 0.1 0.11 $\pm$ 0.15 0.3 $\pm$ 0.5 0.36 $^{\rm +0.09}_{-0.07}$ 30 $\pm$ 5 -2 $\pm$ 2 IV ...
Giant and Supergiant stars with emission lines
HD 323154 B4IIe 15 500 10.2 $\pm$ 0.1  9.3 $\pm$ 0.1 1.10 $\pm$ 0.15 3.4 $\pm$ 0.5 1.1 $^{\rm +0.3}_{-0.2}$ 55 $\pm$ 5 75 $\pm$ 4 I ...
WRAY 15-1104 B1Iae 20 800 11.0 $\pm$ 0.1 10.8 $\pm$ 0.1 0.40 $\pm$ 0.15 1.2 $\pm$ 0.5 20 $^{\rm +7}_{-5}$ 50 $\pm$ 5 60 $\pm$ 5 IV [O I]
Hen 3-1428 B1Iae 20 800 11.3 $\pm$ 0.1 10.9 $\pm$ 0.1 0.61 $\pm$ 0.15 1.9 $\pm$ 0.5 15 $^{\rm +6}_{-4}$ 38 $\pm$ 5 30 $\pm$ 5 I [O I] [N II]
MWC 314 B3Ibe 16 200 11.1 $\pm$ 0.1  9.8 $\pm$ 0.1 1.45 $\pm$ 0.15 4.5 $\pm$ 0.5 1.5 $^{\rm +0.4}_{-0.3}$ 40 $\pm$ 5 65 $\pm$ 10 I [O I] [N II]
HD 320156 B4Ibe 14 900 10.5 $\pm$ 0.1  9.9 $\pm$ 0.1 0.72 $\pm$ 0.15 2.3 $\pm$ 0.5 4.2 $^{\rm +1.0}_{-0.8}$ 35 $\pm$ 5 60 $\pm$ 3 I [O I] [N II]
Hen 3-1347 B5Ibe 13 600 11.9 $\pm$ 0.2 11.5 $\pm$ 0.2 0.56 $\pm$ 0.28 1.8 $\pm$ 0.9 10 $^{\rm +6}_{-4}$ 30 $\pm$ 5 -15 $\pm$ 5 IV [O I]
AS 231 B9Iae 10 300 12.6 $\pm$ 0.6 10.2 $\pm$ 0.1 2.4 $\pm$ 0.6 7.5 $\pm$ 1.9 0.9 $^{\rm +1.3}_{-0.5}$ 28 $\pm$ 5 -25 $\pm$ 5 IV ...
Stars with strong emission line spectrum
WRAY 15-1651 B1-B5 ... 17.0 $\pm$ 0.2 15.8 $\pm$ 0.2 ... ... ... ... ... I [O I]
MWC 930 B5-B9 ... 14.6 $\pm$ 0.5 12.8 $\pm$ 0.5 ... ... ... 70 $\pm$ 10 10 $\pm$ 10 IV [O I]
Dwarf stars without H$\alpha $ in emission
AS 321 A5V 8200 12.0 $\pm$ 0.1 11.3 $\pm$ 0.1 0.60 $\pm$ 0.23 1.9 $\pm$ 0.7 0.31 $^{\rm +0.13}_{-0.09}$ 150 $\pm$ 10 -30 $\pm$ 5 abs. [O I]
Giant and Supergiant stars without H$\alpha $ in emission
WRAY 15-522 G9III 4820 14.3 $\pm$ 0.6 13.4 $\pm$ 0.6 -0.03 $\pm$ 0.8 0.0 $^{\rm +2.6}_{-0.0}$ 3.3 $^{\rm +7.7}_{-2.3}$ <7 -9 $\pm$ 2 abs. [O I]
Th 35-41 M1III 3720 14.5 $\pm$ 0.1 13.1 $\pm$ 0.6 -0.17 $\pm$ 0.6 0.0 $^{\rm +1.5}_{-0.0}$ 5.1 $^{\rm +5}_{-2.6}$ 13 $\pm$ 4 15 $\pm$ 2 abs. ...
WRAY 15-566 M6III 3240 16.0 $\pm$ 0.4 14.2 $\pm$ 0.8 0.31 $\pm$ 0.90 1.0 $\pm$ 2.8 4.6 $^{\rm +13}_{-3.5}$ <7 29 $\pm$ 2 abs. ...
WRAY 15-1650 M6III 3240 13.5 $\pm$ 0.5 11.9 $\pm$ 0.2 0.13 $\pm$ 0.54 0.4 $\pm$ 1.7 2.1 $^{\rm +2.5}_{-1.1}$ <7 -22 $\pm$ 2 abs. ...
WRAY 15-1702 M6III 3240 13.9 $\pm$ 0.2 12.6 $\pm$ 0.2 -0.24 $\pm$ 0.29 0.0 $^{\rm +0.1}_{-0.0}$ 3.4 $^{\rm +0.4}_{-0.4}$ <7 -26 $\pm$ 2 abs. ...
WRAY 15-770 M7III 3150 16.5 $\pm$ 1.0 15.2 $\pm$ 1.0 -0.16 $\pm$ 1.4 0 $^{\rm +3.9}_{-0}$ 11 $^{\rm +62}_{-9.6}$ <7 23 $\pm$ 3 abs. ...
HD 305773 B1Ib 20 800  9.2 $\pm$ 0.1  9.1 $\pm$ 0.1 0.27 $\pm$ 0.15 0.8 $\pm$ 0.5 6.6 $^{\rm +1.6}_{-1.3}$ 27 $\pm$ 5 -2 $\pm$ 1 abs. ...

Notes. Column (3): $T_{\rm eff}$ from Lang et al. 1991 (adapted from Schmidt-Kaler 1982). Columns (4) and (5): photometry in the B and V bands taken from the NOMAD catalog, except for Hen 2-80, Th 17-35, and CD-38 4380 where they are from Vieira et al. (2003) and Hen 3-1121N where they are from the GSC 2.3.2. Columns (6) and (7): Schmidt-Kaler (1982) intrinsic colors and absolute magnitudes of were used to calculate E(B-V) and the distance. The absolute magnitudes for the M6III and M7III stars are absent from the Schmidt-Kaler (1982) tables. We deduced them by linear extrapolation of the MV of the M3III and M4III spectral types. Column (6): $^\star$ in the case of Hen 3-1121N the R = 12.1 $\pm$ 0.4 band magnitude was used to derive E(B-V) using E(B-V)= E(V-R)/0.78. Column (7): no correction for extinction was applied to sources with E(B-V) < 0. Columns (9) and (10): * when the spectra are dominated by emission lines and almost no absorption lines are observed no constrain for $v ~{\rm sin}(i)$ is given and the vr estimate is based on the averaged velocity shift of emission lines (principally He I). Column (11): the type of the H$\alpha $ profile is given following the classification of Reipurth et al. (1996) and Vieira et al. (2003): type I profiles are symmetric without, or with only very shallow absorption features; type II profiles are double-peaked with the secondary peak having more than half of the strength of the primary; type III profiles are double-peaked, with the secondary peak having less than half the strength of the primary; type IV profiles have P Cygni line characteristics. Column (12): F.L. means forbidden lines. [O I] refers to the detection of [O I] lines at 6301, 6365, or 8446 Å; [S II] refers to the [S II] line at 6716 and 6731 Å; [N II] refers to the lines at 6549 and 6585 Å.


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