Table 3
Properties from NH3 (1, 1) and NH3 (2, 2) line spectra.
Source | vlsr | Δva | TKb | σTc | σNT |
(km s-1) | (km s-1) | (K) | (km s-1) | (km s-1) | |
|
|||||
B1-E1 | 7.61 ± 0.02 | 0.998 ± 0.056 | <27 | 0.073 ± 0.007 | 0.417 ± 0.025 |
B1-E2 | 7.67 ± 0.002 | 0.293 ± 0.005 | 10.26 ± 0.36 | 0.071 ± 0.001 | 0.101 ± 0.003 |
B1-E3 | 7.47 ± 0.01 | 0.681 ± 0.030 | <16 | 0.073 ± 0.007 | 0.280 ± 0.015 |
B1-E4 | 7.83 ± 0.01 | 1.078 ± 0.036 | <27 | 0.073 ± 0.007 | 0.451 ± 0.016 |
B1-E5 | 7.57 ± 0.01 | 0.833 ± 0.022 | <19 | 0.073 ± 0.007 | 0.344 ± 0.012 |
B1-E6 | 7.61 ± 0.01 | 0.905 ± 0.032 | <23 | 0.073 ± 0.007 | 0.376 ± 0.015 |
B1-E7 | 7.31 ± 0.01 | 0.708 ± 0.032 | <24 | 0.073 ± 0.007 | 0.290 ± 0.016 |
B1-E8 | 6.78 ± 0.01 | 0.537 ± 0.021 | <20 | 0.073 ± 0.007 | 0.213 ± 0.012 |
B1-E9 | 7.11 ± 0.01 | 0.690 ± 0.038 | < 32 | 0.073 ± 0.007 | 0.282 ± 0.018 |
Notes.
Kinetic temperature towards each source. For B1-E2, we measured the kinetic temperature from NH3 (1, 1) and NH3 (2, 2) line emission. For our other sources, we used a 3σ upper limit for NH3 (2, 2) to estimate the upper limit of TK.
The thermal line width of B1-E2 was determined using the derived kinetic temperature, TK = 10.26 K ± 0.36 K. For the remaining sources, we adopted 11 K, the mean NH3-derived kinetic temperature from Rosolowsky et al. (2008) with an uncertainty of 2 K from the dispersion of the kinetic temperature in that survey (see Enoch et al. 2008).
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