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Table B.4

Total velocity gradients G and FWHM radii RFWHM measured across the cores maps convolved to the largest beam of 29.9′′. The RFWHM are calculatedusing the N2D+(2–1) maps that trace the densest gasa.

Core G RFWHM
(km s−1 pc−1) (pc)
N2D+(2–1) N2H+(1–0) DCO+(2–1) H13CO+(1–0)

2 2.07 ± 0.14 1.89 ± 0.03 2.99 ± 0.07 2.20 ± 0.28 0.019
4 0.51 ± 0.07 1.57 ± 0.036 1.79 ± 0.13 0.026
6 3.78 ± 0.13 4.47 ± 0.03 6.36 ± 0.07 5.76 ± 0.37 0.024
7 6.53 ± 0.10 6.08 ± 0.02 5.12 ± 0.02 5.60 ± 0.09 0.032
8 1.68 ± 0.16 3.97 ± 0.03 3.84 ± 0.19 5.15 ± 0.27 0.030
10 4.19 ± 0.40 4.79 ± 0.06 4.83 ± 0.06 4.74 ± 0.37 0.021
11 1.88 ± 0.26 1.95 ± 0.04 3.96 ± 0.21 2.89 ± 0.32 0.017
12 2.01 ± 0.28 1.99 ± 0.03 4.79 ± 0.13 2.93 ± 0.40 0.025
13 3.15 ± 0.26 3.75 ± 0.09 4.52 ± 0.09 3.38 ± 0.25 0.018
16 0.80 ± 0.22 0.72 ± 0.06 4.15 ± 0.22 1.00 ± 0.46 0.018
17 3.39 ± 0.15 3.12 ± 0.02 2.14 ± 0.07 2.42 ± 0.23 0.026
19 1.54 ± 0.17 1.63 ± 0.02 2.40 ± 0.05 3.31 ± 0.11 0.027

Notes. (a) We do not show the data for core 3 since the poor N2D+(2–1) detection does not allow us to find FWHM.

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