Source | RA [J2000] | Dec [J2000] |
![]() |
![]() ![]() |
d [pc] |
Class 0 | |||||
L1448-mm | 03 25 38.9 | +30 44 05.4 | 77 | 5.3 | 220 |
NGC 1333: | |||||
-IRAS2A | 03 28 55.6 | +31 14 37.1 | 57 | 20a | 220 |
-IRAS4A-SE | 03 29 10.5 | +31 13 31.0 | 43 | 5.8 | 220 |
-IRAS4A-NW | 03 29 10.4 | +31 13 32.3 | - | - | 220 |
-IRAS4B | 03 29 12.0 | +31 13 08.1 | 55 | 3.8b | 220 |
-IRAS4B' | 03 29 12.8 | +31 13 07.0 | - | - | 220 |
L1527 | 04 39 53.9 | +26 03 09.8 | 59 | 2.0 | 140 |
L483 | 18 17 29.9 | -04 39 39.6 | 60 | 9.0 | 200 |
B335 | 19 37 00.9 | +07 34 09.7 | 60 | 3.0 | 250 |
L1157 | 20 39 06.3 | +68 02 16.0 | 42 | 6.0 | 325 |
Class I | |||||
L1489-IRS | 04 04 42.9 | +26 18 56.3 | 238 | 3.7 | 140 |
TMR1 | 04 39 13.9 | +25 53 20.6 | 144 | 3.7 | 140 |
TMC1A | 04 39 35.2 | +25 41 44.4 | 172 | 2.2 | 140 |
GSS30-IRS3 | 16 26 21.7 | -24 22 50.6 | 300 | 14c | 125 |
GSS30-IRS1 | 16 26 22.2 | -24 23 01.9 | - | - | 125 |
WL 12 | 16 26 44.2 | -24 34 48.7 | 440 | 2.6 | 125 |
Elias 29 | 16 27 09.4 | -24 37 20.0 | 350 | 41 | 125 |
IRS 43 | 16 27 26.9 | -24 40 50.6 | 310 | 6.0 | 125 |
IRS 54 | 16 27 51.8 | -24 31 45.4 | 740 | 2.5 | 125 |
IRS 63 | 16 31 35.7 | -24 01 29.6 | 530 | 3.3 | 125 |
aFor NGC 1333-IRAS2A Evans et al. (2009) quote a luminosity of 76 .
Estimating the luminosity from scaling the 70
m flux using the approach of Dunham et al. (2008) gives a luminosity of 19.6
,
which agrees well with previous estimates from modeling the SED in the range 16-20
.
The higher luminosity in the c2d compilation is a result of the SED of IRAS2A being unconstrained at 24
m (Dunham, priv. comm) - and we therefore adopt a luminosity of 20
for this source. b
The Spitzer maps of NGC 1333-IRAS4B shows significant emission
from a nearby outflow shock within the typical single-dish beam. As
total luminosity for this source, we adopt the sum of the two
components, SSTc2d J032912.06+311305.4 and SSTc2d J032912.06+311301.7,
from Evans et al. (2009). c
The emission from GSS30-IRS3 (LFAM1) and GSS30-IRS1 are not separated
in the Spitzer catalog (the latter dominates the emission and its
luminosity is quoted here).
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