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Table 2

Properties of the submillimetre cores detected at 870 μm in Cha II.

Core RAa Deca S 870μm b rms Mass Deconvolved c n core n crit d Sep.e Counterpart?
(J2000) (J2000) (mJy) (mJy) (M) ang. size (cm-3) (cm-3) (“)

ChaII-APEX-A 12:53:30.5 –77:11:07 26 5 0.016 Point-like ... 4.3 × 107 7′′, 10′′ No (Background star)
ChaII-APEX-B 12:54:17.3 –77:10:23 26 5 0.016 Point-like ... 4.3 × 107 15′′ No (Background star)
ChaII-APEX-C 12:56:03.3 –77:11:43 36f 6 0.022 35′′ 2.2 × 104 2.3 × 107 12′′, 14′′ No (Background star)
ChaII-APEX-D 12:53:42.6 –77:15:11 109 5 0.066 Point-like ... 2.5 × 106 1′′ Yes (YSO IRAS 12500-7658)
ChaII-APEX-E 12:53:39.0 –77:16:35 460 f 5 0.279 75′′ 2.8 × 104 1.4 × 105 ... No
ChaII-APEX-F 12:54:21.9 –77:06:59 35 5 0.021 Point-like ... 2.5 × 107 ... No
ChaII-APEX-G 12:54:12.3 –77:06:47 130f 5 0.079 45′′ 3.7 × 104 1.7 × 106 11′′ No (Background star)
ChaII-APEX-H 12:54:40.8 –77:04:35 49f 6 0.030 35′′ 3.1 × 104 1.2 × 107 4′′, 14′′, 16′′ No (Background star)
ChaII-APEX-I 12:54:27.7 –77:04:27 30 6 0.018 Point-like ... 3.4 × 107 13′′ No (Background star)
ChaII-APEX-J 12:53:44.8 –77:04:43 39f 6 0.024 40′′ 1.5 × 104 1.9 × 107 18′′ No (Background star)
ChaII-APEX-K 12:53:17.3 –77:07:11 1745 4 1.059 Point-like ... 9.7 × 103 0.5′′ Yes (YSO DK Cha)
ChaII-APEX-L 12:52:55.8 –77:07:35 78 5 0.047 Point-like ... 4.9 × 106 1′′ Yes (Proto-BD candidate)
ChaII-APEX-M 12:52:39.0 –77:07:59 3700f 4 2.246 80′′ 1.8 × 105 2.2 × 103 ... No
ChaII-APEX-N 12:51:55.8 –77:08:43 30 5 0.018 Point-like ... 3.4 × 107 16′′ No (Background star)
ChaII-APEX-O 12:51:39.0 –77:08:55 260f 6 0.158 55′′ 4.0 × 104 4.4 × 105 13′′, 16′′ No (Background star)

Notes.

(a)

Position of the maximum emission of the cores. Units of right ascension are hours, minutes, and seconds. Units of declination are degrees, arcminutes, and arcseconds.

(b)

Flux density computed above 3σ emission.

(c)

Deconvolved size after fitting a Gaussian to the cores. The averaged of the major and minor axis is represented.

(d)

Critical density of the core, calculated following the equation in Sect. 4.4.

(e)

Separation of the counterpart candidates to the nominal position of the submillimetre core.

(f)

For cores showing extended emission we applied a specific data processing (using option “extended” in CrUSH) to avoid filtering out extended structures.

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