Table 1
List of observed sources and spectral energy distribution parameters.
α | δ | V lsr b | D | SED fitd | L bol e | L/M | ||||||
|
||||||||||||
# | Sourcea | (J2000) | (J2000) | (km s-1) | (kpc) | IRc | β | Tdust (K) | M (M⊙) | (L⊙) | (L⊙M⊙-1) | |
|
||||||||||||
01 | 18151−1208_1 | 18:17:58.0 | −12:07:27.0 | +33.0 | 3.0 | L | 1.7 | 32 | 478 | 26 090 | 54.6 | |
02 | G19.27+0.1M2 | 18:25:52.6 | −12:04:48.0 | +26.9 | 2.4 | D | 2.5 | 35 | 77 | 157 | 2.0 | |
03 | G19.27+0.1M1 | 18:25:58.5 | −12:03:59.0 | +26.5 | 2.4 | D | 1.3 | 22 | 193 | 374 | 1.9 | |
04 | 18236−1205 | 18:26:25.4 | −12:03:51.4 | +26.5 | 2.5 | L | 1.0 | 29 | 935 | 4507 | 4.8 | |
05 | 18264−1152 | 18:29:14.4 | −11:50:21.3 | +43.7 | 3.5 | L | 1.3 | 27 | 1634 | 11 910 | 7.3 | |
06 | G23.60+0.0M1 | 18:34:11.6 | −08:19:06.0 | +106.5 | 6.2 | D | 2.0 | 18 | 1820 | 5207 | 2.9 | |
07 | 18 316−0602 | 18:34:20.5 | −05:59:30.4 | +42.5 | 3.1 | L | 1.2 | 33 | 1613 | 31 820 | 19.7 | |
08 | G23.60+0.0M2 | 18:34:21.1 | −08:18:07.0 | +53.5 | 3.9 | D | 1.9 | 23 | 287 | 3049 | 10.6 | |
09 | G24.33+0.1M1 | 18:35:07.9 | −07:35:04.0 | +113.6 | 6.7 | D | 2.2 | 23 | 2674 | 48 050 | 18.0 | |
10 | G34.43+0.2M1f | 18:53:18.0 | +01:25:23.0 | +57.9 | 3.7 | D | 1.8 | 26 | 1369 | 24 050 | 17.6 | |
11 | 18507+0121 | 18:53:19.6 | +01:24:37.1 | +57.6 | 3.7 | L | 1.0 | 29 | 3065 | 14 530 | 4.7 | |
12 | G34.43+0.2M3 | 18:53:20.4 | +01:28:23.0 | +59.2 | 3.7 | D | 1.5 | 21 | 612 | 1357 | 2.2 | |
13 | 19095+0930 | 19:11:54.0 | +09:35:52.0 | +43.9 | 3.3 | L | 1.6 | 33 | 971 | 50 680 | 52.2 | |
14 | 23139+5939 | 23:16:11.1 | +59:55:30.8 | −44.5 | 4.8 | L | 1.6 | 30 | 972 | 26 040 | 26.8 |
Notes.
Name of sources starting with numbers (e.g., 18151−1208) refer to the IRAS name (Neugebauer et al. 1984).
Systemic velocity (VLSR) derived from the hyperfine fit to the N2H+ (1–0) and C2H (1–0) lines (see Sect. 3.1).
Sources classified as IR-luminous (IRL) or IR-dark (IRD) according to its emission or not at mid-IR wavelengths according to López-Sepulcre et al. (2010).
Parameters obtained from the single-temperature, modified black body fit to the spectral energy distribution (see Sect. 3.3).
Bolometric luminosity derived by integrating over the full observed spectral distribution (see Sect. 3.3).
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