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Table 2

Properties of the continuum mm sources in IRAS 19410+2336.

Source RA Dec I ν S ν T k a Mass A v
(J2000) (J2000) ( mJy beam-1) (mJy) (K) (M⊙) (1023 cm-2) (103 mag) Flags
1.4 mm with a 1.2′′ × 0.8′′ beam
1-s ... 19 43 11.553 23 44 14.15 4.8 ... 35 1.5 8.2 0.9 u
2-s ... 19 43 11.093 23 44 09.90 5.7 ... 35 1.7 9.6 1.0 u
3-s ... 19 43 10.989 23 44 08.64 8.1 8.3 35 2.5 14 1.5
4-s ... 19 43 11.387 23 44 07.29 5.3 ... 35 1.6 9.0 1.0 u
5-s ... 19 43 11.286 23 44 07.49 6.2 ... 35 1.9 10 1.1 u
6-s ... 19 43 11.182 23 44 07.78 1.1 16 35 4.9 19 2.0
7-s ... 19 43 11.093 23 44 07.41 7.6 7.7 35 2.4 13 1.4
8-s ... 19 43 10.989 23 44 07.33 5.6 ... 35 1.7 9.4 1.0 u
9-s ... 19 43 11.191 23 44 06.68 1.0 14 35 4.3 17 1.8
10-s ... 19 43 11.342 23 44 05.37 7.2 11 35 3.4 12 1.3
11-s ... 19 43 11.229 23 44 05.37 5.6 ... 35 1.7 9.5 1.0 u
12-s ... 19 43 11.357 23 44 02.39 1.3 24 45 5.5 17 1.8
13-s ... 19 43 11.191 23 44 03.00 4.2 75 90 8.1 25 2.7
14-s ... 19 43 10.950 23 44 02.15 4.6 ... 35 1.4 7.8 0.8 u
15-s ... 19 43 10.837 23 44 01.94 4.8 ... 35 1.5 8.1 0.9 u
16-s ... 19 43 10.614 23 44 01.33 7.3 ... 35 2.2 13 1.4 u
17-s ... 19 43 10.385 23 44 02.15 5.1 ... 35 1.6 8.7 1.0 u
18-s ... 19 43 11.539 23 43 57.94 4.6 ... 35 1.4 7.8 0.8 u
19-s ... 19 43 11.458 23 44 57.17 5.3 ... 35 1.6 9.0 1.0 u
1-n ... 19 43 10.801 23 45 08.26 3.4 ... 35 1.0 5.8 0.6 u
2-n ... 19 43 10.728 23 45 07.41 6.1 ... 35 1.9 11 1.0 u
3-n ... 19 43 10.743 23 45 06.51 4.5 ... 35 1.4 7.6 0.8 u
4-n ... 19 43 10.706 23 44 58.42 2.7 32 60 5.3 25 2.7
5-n ... 19 43 10.636 23 44 59.48 3.6 ... 50 0.7 4.1 0.4 u
6-n ... 19 43 10.524 23 44 58.45 4.7 ... 35 1.4 7.9 0.8 u
7-n ... 19 43 10.469 23 45 00.2 3.6 ... 35 1.1 6.1 0.6 u
3 mm with a 2.2′′ × 1.6′′ beam
1-s ... 19 43 11.558 23 44 14.41 5.1 ... 40 19.9 32 3.4 u
20-s ... 19 43 11.073 23 44 12.23 3.1 ... 40 12.1 19 2.1 u, n
c3mm-sI ... 19 43 10.986 23 44 08.67 4.8 6.7 40 26.2 29 3.1 c(2, 3, 8-s)
c3mm-sII ... 19 43 11.170 23 44 07.64 6.6 13 40 50.8 40 4.2 c(5, 6, 7, 9-s)
c3mm-sIII ... 19 43 11.206 23 44 03.29 17.7 48 40 187.5 102 10.8 c(10, 11, 12, 13-s)
16-s ... 19 43 10.587 23 44 01.71 2.9 ... 40 11.2 18 1.9 u
17-s ... 19 43 10.382 23 44 02.20 3.5 3.9 40 15.2 22 2.3
21-s ... 19 43 12.066 23 44 05.76 2.0 ... 40 7.9 12 1.3 u, n
22-s ... 19 43 12.037 23 44 03.68 2.0 ... 40 7.7 12 1.3 u, n
c3mm-nI ... 19 43 10.746 23 45 07.63 3.2 ... 40 12.7 20 2.1 u, c(1, 2, 3-n)
8-n ... 19 43 10.746 23 45 05.01 1.9 ... 40 7.5 12 1.2 u, n
c3mm-nII ... 19 43 10.707 23 44 58.54 5.1 7.4 40 29.0 31 3.3 c(4, 5-n)
6-n ... 19 43 10.573 23 44 58.47 2.6 ... 40 10.2 16 1.7 u
7-n ... 19 43 10.480 23 45 00.61 2.2 ... 40 8.5 13 1.4 u

Notes. The last column indicates unresolved cores (u) and detections at 3 mm without a 1.4 mm counterpart (n). The c(X, Y, Z) flag indicates that the source is the unresolved combination of sources X, Y, and Z. If the source is unresolved, its mass in Col. 7 is calculated with the peak intensity value of Col. 4.

(a)

Derived from the H2CO emission, the 3 mm temperatures are the average in the region (see Sect. 4.1.2). The values for the 1.4 mm cores are the same as in Table 3, and are repeated here just for reading convenience.

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