Position |
![]() |
![]() |
Deconv. sizec | PAc | M
![]() |
||
Source |
![]() |
![]() |
(m
![]() |
(mJy) | (
![]() |
(![]() |
(
![]() |
MM1-maine | 00 14 26.051 | 64 28 43.69 |
![]() |
![]() |
![]() |
![]() |
1.46 |
![]() |
![]() |
||||||
MM1-S | 00 14 26.065 | 64 28 42.26 | ![]() |
![]() |
![]() |
![]() |
0.20 |
MM1-SW | 00 14 25.861 | 64 28 42.25 | ![]() |
![]() |
![]() |
![]() |
0.24 |
Notes. (a) Synthesized
beam of the uniform-weighted map is
with
PA=+66
.
The rms noise level of the map is 1.0 mJy beam-1.
(b) Primary beam
corrected. Error in intensity and flux density as in Table 2.(c) Deconvolved
sizes and PA obtained from a fit with two Gaussian for MM1-main, and
one single Gaussian for MM1-S and MM1-SW. (d) Masses
derived assuming a dust mass opacity coeffecient at 1.2 mm of
0.9 g cm-1 (agglomerated
grains with thin ice mantles in cores of densities
106 cm-3,
Ossenkopf & Henning 1994),
and a dust temperature of 30 K. The uncertainty in the masses
due to the opacity law is estimated to be of a factor of 2. (e) Throughout
all the text, we refer to MM1-main as MM1, for simplicity.
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