Table 1
Continuum peak emission at 1.4 mm, detected in Perseus using the CALYPSO survey, where glycolaldehyde emission has been searched for.
Source | α(J2000)a | δ(J2000)a | Vsys a | d b | F1.4 mm | Lintc | HPB Wsyn | |
(hms) | (°′″) | (km s-1) | (pc) | (mJy/beam) | (L⊙) | ″×″(°) | ||
|
||||||||
1.4 mm | 1.3 mm | |||||||
|
||||||||
L1448-2A | 03:25:22.406 | +30 45 13.28 | +4.2 | 232 | 31 | 2.7 | 0![]() ![]() |
1![]() ![]() |
L1448-NB | 03:25:36.364 | +30 45 14.84 | +4.7 | 232 | 25 | 4.1 | 0![]() ![]() |
0![]() ![]() |
L1448-NA | 03 25 36.503 | +30 45 21.87 | +4.7 | 232 | 139 | – | 0![]() ![]() |
0![]() ![]() |
L1448-C | 03 25 38.878 | +30 44 05.32 | +5.2 | 232 | 102 | 6.8 | 0![]() ![]() |
0![]() ![]() |
IRAS2A3 | 03 28 55.514 | +31 14 34.84 | +7.3 | 235 | 16 | – | 0![]() ![]() |
0![]() ![]() |
IRAS2A1 | 03 28 55.575 | +31 14 37.05 | +7.3 | 235 | 99 | 26.7 | 0![]() ![]() |
0![]() ![]() |
IRAS2A2 | 03 28 55.677 | +31 14 35.56 | +7.3 | 235 | 12 | – | 0![]() ![]() |
0![]() ![]() |
SVS13-B | 03 29 03.075 | +31 15 51.71 | +8.4 | 235 | 122 | 1–2c | 1![]() ![]() |
0![]() ![]() |
SVS13-A | 03 29 03.759 | +31 16 03.74 | +8.4 | 235 | 123 | 24.5 | 1![]() ![]() |
0![]() ![]() |
IRAS4A2 | 03 29 10.429 | +31 13 32.10 | +7.2 | 235 | 284 | – | 1![]() ![]() |
0![]() ![]() |
IRAS4A1 | 03 29 10.531 | +31 13 30.96 | +7.2 | 235 | 795 | 2.8 | 1![]() ![]() |
0![]() ![]() |
IRAS4B1 | 03 29 12.012 | +31 13 08.07 | +6.7 | 235 | 449 | 1.0 | 1![]() ![]() |
0![]() ![]() |
IRAS4B2 | 03 29 12.840 | +31 13 06.98 | +6.7 | 235 | 53 | – | 1![]() ![]() |
0![]() ![]() |
Notes.
Positions of the 1.3 mm continuum peak emission and systemic velocities are extracted from the CALYPSO dataset (Codella et al. 2014; Santangelo et al. 2015; Anderl et al. 2016; Maury et al., in prep.).
Internal luminosities were derived from the observed flux at 70 μm (Dunham et al. 2008), a wavelength at which Herschel Gould Belt survey observations (André et al. 2010) provide data at 8″ spatial resolution (see also Ladjelate et al., in prep.). The internal luminosity of SVS13-B is more uncertain due to the proximity to SVS13-A.
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