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Source | Position (1.3 mm) | Peak flux | FWHM1 | Flux density2 | Separation3 | |
![]() |
![]() |
(mJy/beam) | (arcsec) | (mJy) | (AU) | |
L1448-C | 03:25:38.87 | 30:44:05.3 | 59 ![]() |
0.9 ![]() |
57 ![]() |
- |
L1448-C / South1 | 03:25:38.95 | 30:44:03.2 | 11 ![]() |
0.7 ![]() |
11 ![]() |
600 |
NGC 1333-IRS2A | 03:28:55.56 | 31:14:37.1 | 26 ![]() |
0.55 ![]() |
18 ![]() |
- |
NGC 1333-IRS2A / SE | 03:28:56.00 | 31:14:33.1 | 7 ![]() |
0.23 ![]() |
4 ![]() |
1900 |
IRAM 04191 | 04:21:56.90 | 15:29:46.1 | 2 ![]() |
0.28 ![]() |
0.9 ![]() |
- |
L1527 | 04:39:53.87 | 26:03:09.8 | 50 ![]() |
0.42 ![]() |
65 ![]() |
- |
L1521-F | 04:28:38.94 | 26:51:35.2 | 1 ![]() |
0.65 ![]() |
0.8 ![]() |
- |
Notes. (1) FWHM
diameter is computed from a circular Gaussian fit to the visibilities. (2) Flux integrated above the 3 ![]() (3) Projected distance to the primary source. |
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