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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. 

(a)

The velocity FWHM from the best-fit models uncorrected for channel resolution.

(b)

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.

(c)

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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