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Table 3

Results from Gaussian fits, Tl, ΔV, and VLSR for the emission, calculated peak opacities, τp, integrated opacities, , and column densities of the absorbing material in respective lower state, Nl.

Freq. T l a ΔV b V LSR τ p c c N l d
(GHz) (K) (km s-1) (km s-1) (km s-1) (cm-2)

o-NH3 572.498 −0.7 ± 0.1 3.8 ± 0.3 60.3 ± 0.3 1.3 5.4 2.0e13
−0.1 ± 0.1 2.1 ± 0.9 61.4 ± 0.3 0.2 0.4 1.5e12
1.85 ± 0.01 4.2 ± 0.07 55.55 ± 0.04 ... ...
0.14 ± 0.01 10.0 ± 0.8 69.5 ± 0.3 ... ...
1214.853 −1.7 ± 0.1 4.5 ± 0.9 60.5 ± 0.4 0.5 2.3 1.3e13
−0.6 ± 0.4 2.4 ± 0.7 63.1 ± 0.3 0.2 0.4 2.2e12
1.2 ± 0.1 4.3 ± 0.4 55.9 ± 0.3 ... ...
1763.524 −0.92 ± 0.2 2.2 ± 0.5 60.8 ± 0.1 0.2 0.4 2.2e12
−1.7 ± 0.1 2.2 ± 0.1 62.8 ± 0.1 0.3 0.7 4.1e12
0.10 ± 0.08 4.2 ± 18 56.8 ± 6.7 ... ...

p-NH3 1168.452 −3.2 ± 0.1 4.3 ± 0.3 60.6 ± 0.1 1.3 5.7 4.2e13
−0.4 ± 0.3 3.1 ± 0.7 63.8 ± 0.6 0.1 0.3 2.6e12
1.03 ± 0.04 3.1 ± 0.2 55.8 ± 0.1 ... ...
1215.246 −3.3 ± 0.3 4.3 ± 0.3 60.4 ± 0.2 1.4 5.4 4.0e13
−0.9 ± 0.6 3.1 ± 0.7 63.5 ± 0.8 0.2 0.9 6.6e12
1.07 ± 0.04 3.5 ± 0.3 55.8 ± 0.1 ... ...
1763.601 −1.04 ± 0.05 2.3 ± 0.2 60.6 ± 0.2 0.2 0.4 2.8e12
−1.60 ± 0.05 2.2 ± 0.1 62.9 ± 0.2 0.3 0.6 4.4e12
0.29 ± 0.02 3.9 ± 0.8 56.8 ± 0.2 ... ...
1763.823 −2.85 ± 0.04 4.1 ± 0.2 60.9 ± 0.1 0.6 2.5 2.7e13
−1.1 ± 0.2 2.0 ± 0.2 63.3 ±0.1 0.2 0.4 4.2e12
0.27 ± 0.04 1.7 ± 0.4 56.2 ± 0.1 ... ...

Notes.

(a)

Amplitude of Gaussian fit. A negative value represents absorption and a positive value emission.

(b)

Line width from Gaussian fit.

(c)

Estimated with Eq. (1).

(d)

Estimated with Eq. (2), and listed as upper limits for components that are not statistically significant in the Gaussian fitting.

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