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Table 5

Thermal and non-thermal parameters.

NH3 H2CO


Sources σT σNT as Rp σT σNT as Rp
km s-1 km s-1 km s-1 km s-1 km s-1 km s-1

G5.89-0.39 0.13 1.68 0.36 0.046 0.10 3.17 0.38 0.014
G5.90-0.44 0.12 0.92 0.32 0.121 0.08 2.09 0.34 0.027
G5.97-1.36 0.13 0.87 0.35 0.160 ... 0.90 ... ...
G6.91-0.22 0.08 0.75 0.22 0.090 ... 2.20 ... ...
G9.04-0.52 0.08 0.57 0.22 0.144 ... 0.82 ... ...
G9.21-0.20 0.09 0.70 0.24 0.121 ... 1.18 ... ...
G9.88-0.75 0.10 0.80 0.27 0.115 ... 1.57 ... ...
G10.99-0.08 0.08 0.74 0.20 0.074 ... ... ... ...
G11.92-0.61 0.10 0.70 0.26 0.142 ... 2.41 ... ...
G12.43-1.11 0.11 0.82 0.31 0.141 ... 1.44 ... ...
G12.68-0.18 0.12 1.02 0.32 0.099 ... 2.74 ... ...
G12.91-0.26 0.11 1.27 0.30 0.056 0.11 2.40 0.39 0.026
G13.28-0.30 0.08 0.53 0.21 0.153 ... ... ... ...
G14.20-0.19 0.10 1.14 0.26 0.051 0.12 1.96 0.44 0.051
G14.33-0.64 0.11 1.25 0.29 0.053 0.11 1.72 0.39 0.052
G15.66-0.50 0.11 1.08 0.28 0.068 ... 2.03 ... ...
G17.10+1.02 0.17 0.72 0.44 0.372 ... 1.25 ... ...
G18.21-0.34 0.09 0.68 0.24 0.120 ... 2.13 ... ...
G19.01-0.03 0.09 0.63 0.25 0.161 ... 2.57 ... ...
G22.55-0.52 0.09 0.58 0.23 0.161 ... 1.82 ... ...
G28.61-0.03 0.14 1.06 0.36 0.119 ... 2.63 ... ...
G28.86+0.07 0.15 1.38 0.39 0.082 0.10 2.59 0.41 0.025
G30.24+0.57 0.13 1.39 0.35 0.063 ... ... ... ...
G30.70-0.07 0.11 1.61 0.29 0.033 0.10 2.07 0.36 0.030
G31.40-0.26 0.13 1.44 0.34 0.055 0.10 2.12 0.40 0.035
G31.70-0.49 0.07 0.44 0.19 0.191 ... ... ... ...
G34.37-0.66 0.07 0.32 0.18 0.323 ... ... ... ...
G35.03+0.35 0.12 1.20 0.33 0.075 0.11 2.27 0.39 0.030
G35.19-0.74 0.11 1.33 0.30 0.049 0.10 2.86 0.31 0.012
G37.87-0.40 0.12 2.11 0.33 0.025 ... 2.67 ... ...

Notes. Columns 2–5 and 6–9 are thermal linewidth, non-thermal velocity dispersion, thermal sound speed, and the ratio of thermal to nonthermal pressure obtained from NH3 (1, 1) and para-H2CO (303–202) with kinetic temperatures derived from the NH3 (2, 2)/(1, 1) and para-H2CO (321–220/303–202) line intensity ratios, respectively. Para-H2CO non-thermal velocity dispersions without kinetic temperatures are deduced from σNT = ΔV/2.355 (Pan & Padoan 2009), where ΔV is the measured FWHM linewidth.

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