Table 2
MDC and HMPC samples.
Name | RA | Dec | Size | d | S int | FWHM a | M 20 K b | ⟨ nH2 ⟩ c | Remarks |
(J2000) | (J2000) | [″×″] | [kpc] | [mJy] | [pc] | [M⊙] | [107cm-3] | ||
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | ||
|
|||||||||
N1 MDC | 18:47:47.0 | –1:54:26 | 6.2 × 4.0 | 6 | 135.2 | 0.088 | 2128 ± 53 | 10.35 ± 0.26 | |
N2 MDC | 18:47:46.4 | –1:54:32 | 5.6 × 4.0 | 6 | 34.7 | 0.076 | 545 ± 59 | 4.19 ± 0.45 | |
N3 MDC | 18:47:45.7 | –1:54:11 | 5.2 × 4.0 | 6 | 13.4 | 0.066 | 211 ± 38 | 2.43 ± 0.47 | |
N4 MDC | 18:47:44.6 | –1:54:40 | 5.0 × 4.1 | 6 | 9.7 | 0.074 | 153 ± 38 | 1.92 ± 0.47 | |
N5 MDC | 18:47:45.8 | –1:54:33 | 5.4 × 4.1 | 6 | 9.7 | 0.074 | 153 ± 27 | 1.24 ± 0.22 | |
N6 MDC | 18:47:44.9 | –1:54:44 | 5.3 × 4.0 | 6 | 8.9 | 0.069 | 141 ± 36 | 1.45 ± 0.37 | |
N7 MDC | 18:47:46.5 | –1:54:21 | 5.1 × 4.0 | 6 | 7.1 | 0.063 | 111 ± 26 | 1.45 ± 0.33 | |
N8 MDC | 18:47:44.0 | –1:54:36 | 5.0 × 4.0 | 6 | 6.7 | 0.061 | 105 ± 19 | 1.56 ± 0.28 | |
N9 MDC | 18:47:48.5 | –1:54:34 | 4.6 × 4.0 | 6 | 3.5 | 0.048 | 56 ± 17 | 1.64 ± 0.49 | |
N10 MDC | 18:47:46.4 | –1:54:52 | 4.9 × 4.0 | 6 | 5.6 | 0.059 | 88 ± 26 | 1.50 ± 0.45 | |
N11 MDC | 18:47:47.8 | –1:54:20 | 5.8 × 4.0 | 6 | 7.3 | 0.080 | 115 ± 24 | 0.75 ± 0.16 | |
|
|||||||||
N12 dense core | 18:47:49.6 | –1:54:00 | 5.2 × 4.1 | 6 | 1.3 | – | 21 ± 5 | – | aperture extraction |
N1a HMPC | 18:47:47.0 | –1:54:26 | 2.8 × 2.2 | 6 | 1900 | 0.033 | 1080 ± 35 | 104 ± 3.4 | 1 mm extraction |
N1b HMPC | 18:47:46.8 | –1:54:29 | 3.4 × 2.2 | 6 | 700 | 0.047 | 395 ± 30 | 12.9 ± 1 | 1 mm extraction |
|
|||||||||
Cygnus X MDCs | 1.4d | – | ~0.11d | ~60de | ~0.18de | Motte et al. (2007) | |||
SDC335-MM1 HMPC | 3.25 | – | ~0.054 | ~343e | ~7e | Peretto et al. (2013) | |||
G0.22&G0.24 HMPCs | 3.6–6.5 | – | ~0.034 | ~8.7e | ~1e | Rathborne et al. (2007) | |||
G11.110.12 HMPCs | 3.6 | – | ~0.025 | ~10.6e | ~2.94e | Wang et al. (2014) | |||
Cygnus X HMPCs | 1.4d | – | ~0.016d | ~12de | ~3.6de | Bontemps et al. (2010) |
Notes.
M20 K masses and relative uncertainties are calculated with Eq. (1) from integrated fluxes Sint (Col. 4) and errors measured by Getsources, except when mentioned in remarks. The errors do not consider the absolute uncertainties such as flux calibration, temperature, and emissivity assumptions.
Sizes, masses, and densities have been recalculated with a distance to Cygnus X of 1.4 kpc from the Sun (Rygl et al. 2012).
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