\begin{table}%t3 \caption{\label{tab3}Established spectral type, literature photometry, estimated distance, radial and projected rotational velocity, observed~H$\alpha$ and forbidden line emission.}\vspace*{2mm} \par %\centering \par \begin{tabular}{l c c c c c c c c c c c c c c c } \hline\hline \noalign{\smallskip} & & $T_{\rm eff}$ & $B$ & $V$ & $E(B-V)$ & $A_V$ & $d_{\rm phot}$ & $v ~{\rm sin}(i)$ & $v_r$ & \\ 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) \\ \hline \multicolumn{12}{c}{\it 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 & [\ion{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 & [\ion{O}{i}] [\ion{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 & [\ion{O}{i}] [\ion{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 & [\ion{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 & [\ion{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 & [\ion{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 & [\ion{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 & [\ion{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 & [\ion{O}{i}][\ion{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 & [\ion{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 & [\ion{O}{i}] \\[2pt] \hline \multicolumn{12}{c}{\it 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 & [\ion{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 & ... \\[2pt] \hline \multicolumn{12}{c}{\it 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 & [\ion{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 & [\ion{O}{i}] [\ion{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 & [\ion{O}{i}] [\ion{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 & [\ion{O}{i}] [\ion{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 & [\ion{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 & ... \\[2pt] \hline \multicolumn{12}{c}{\it Stars with strong emission line spectrum}\\ WRAY 15-1651 & B1-B5 & ... & 17.0 $\pm$ $0.2$ & 15.8 $\pm$ $0.2$ & ... & ... & ... & ... & ... & I & [\ion{O}{i}] \\ MWC 930 & B5-B9 & ... & 14.6 $\pm$ $0.5$ & 12.8 $\pm$ $0.5$ & ... & ... & ... & 70 $\pm$ $10$ & 10 $\pm$ $10$ & IV & [\ion{O}{i}] \\[2pt] \hline \multicolumn{12}{c}{\it 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. & [\ion{O}{i}] \\[2pt] \hline \multicolumn{12}{c}{\it 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. & [\ion{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. & ...\\[2pt] \hline \end{tabular} \tablefoot {Column~(3): $T_{\rm eff}$ from Lang et~al. 1991 (adapted from \mbox{Schmidt-Kaler} \cite{Schm82}). 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. (\cite{Viei03}) and Hen~3-1121N where they are from the GSC~2.3.2. Columns~(6) and~(7): \mbox{Schmidt-Kaler} (\cite{Schm82}) 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 \mbox{Schmidt-Kaler} (\cite{Schm82}) tables. We deduced them by linear extrapolation of the~$M_V$ 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~$v_r$ estimate is based on the averaged velocity shift of emission lines (principally~\ion{He}{i}). Column~(11): the~type of the H$\alpha$~profile is given following the classification of Reipurth et~al. (\cite{Reip96}) and Vieira et~al. (\cite{Viei03}): 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. [\ion{O}{i}]~refers to the detection of [\ion{O}{i}]~lines at~6301, 6365, or 8446~\AA; [\ion{S}{ii}] refers to the [\ion{S}{ii}]~line at~6716 and 6731~\AA; [\ion{N}{ii}]~refers to the lines at~6549 and 6585~\AA.} \vspace*{3mm}\end{table}