Open Access

Table 1

Properties of the sample.

Name α2000 (a) δ2000 Cloud Dist. (b) Outflow PA (c), (5) Tbol (d) Lint (e) Menv (f)
[h:m:s] [°:′:′′] (pc) (°) (K) (L) (M)
NGC 1333-IRAS 2A1 03:28:55.57 31:14:37.07 Perseus 293 (1) +205 41 (6) 47 7.9 (14)
NGC 1333-IRAS 4A1 03:29:10.54 31:13:30.98 Perseus 293 (1) +180 29 (11) 4.7 12.2 (18)
NGC 1333-IRAS 4B 03:29:12.02 31:13:08.02 Perseus 293 (1) +167 28 (11) 2.3 4.7 (18)
L1448-2A 03:25:22.40 30:45:13.26 Perseus 293 (1) −63 43 (11) 4.7 1.8 (12)
L1448-C 03:25:38.87 30:44:05.33 Perseus 293 (1) −17 47 (11) 11 1.9 (18)
L1448-NB1 03:25:36.38 30:45:14.77 Perseus 293 (1) −80 57 (11) 3.9 4.9 (18)
SVS13B 03:29:03.08 31:15:51.74 Perseus 293 (1) +167 20 (10) 3.1 2.8 (13)
L1527 04:39:53.87 26:03:09.66 Taurus 140 (3) +60 59 (6) 0.9 1.2 (15)
Serpens Main S68N 18:29:48.09 01:16:43.41 Serp. Main 436 (g), (2) −45 58 (7) 11 11 (16)
Serpens Main SMM4 18:29:56.72 01:13:15.65 Serp. Main 436 (g), (2) +30 26 (8) 2.2 7.7 (16)
Serpens South MM18 18:30:04.12 −02:03:02.55 Serp. South 350 (g) +188 35 (9) 29 5.4 (17)
L1157 20:39:06.27 68:02:15.70 Cepheus 352 (4) 163 42 (6) 4.0 3.0 (15)

Notes. (a) Peak position of CALYPSO 1.3 mm continuum emission as derived by Maury et al. (2019). (b) Distance to the hosting cloud. (c)Position angle of the outflow derived from the CALYPSO molecular line emission maps. (d) Bolometric temperature. (e)Internal luminosity. The Lint were calculated from the analysis of the Herschel maps from the Herschel Gould Belt survey (André et al. 2010; Ladjelate, in prep.) and rescaled to the distances used in this analysis. (f) Envelope mass. The Menv were rescaled to the distances used in this analysis. (g)A mean distance of 436 pc for the Serpens Cloud has been determined by Ortiz-León et al. (2018b) using the Gaia-DR2 results and seems to correspond to the average distance determined from the Main cloud or the star-forming region W40. Ongoing work reanalyzing the Gaia data toward Serpens South seems, however, to suggest a first layer of extinction around 300–350 pc while its associated young stellar objects could be distributed in a larger extinction layer up to distances of 350 pc (Palmeirim et al., in prep.). We use this new distance for the paper. As we are working on flux ratios, this does not affect the slope we present for SerpS-MM18. This, however, has an impact on the envelope mass discussed in Sect. 6, which would be higher by a factor of 1.6 if the distance is 436 pc.

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.