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Table 1

Line parameters of DCN (2–1) and H13CN (2–1) derived in the five regions depicted in Fig. 1 and from the spectra integrated over the whole emission of DCNa.

Tmbd v v LSR N Dfracb
(× 1011 cm-2) (× 10-2)
(K  km s-1) ( km s-1) 10–70 K 10–70 K

E-wall (B0e)
DCN (2–1) 0.71(0.11) 0.15 2.7(0.4)−7.2(1.1) 0.47(0.12)−0.54(0.14)
H13CN (2–1) 2.33(0.41) − 1.86 7.5(1.3)−17.1(2.8)

B1a
DCN (2–1) 0.79(0.12) 1.16 3.0(0.5)−8.0(1.2) 0.32(0.07)−0.37(0.08)
H13CN (2–1) 3.84(0.65) − 0.95 12.4(2.1)−28.2(4.8)

B1e
DCN (2–1) 0.24(0.05) 1.15 0.9(0.3)−2.4(0.4) 0.08(0.03)−0.09(0.03)
H13CN (2–1) 4.83(0.75) − 0.89 15.6(2.5)−35.5(5.7)

B1c
DCN (2–1) 0.57(0.09) 1.13 2.2(0.3)−5.8(0.9) 0.26(0.06)−0.30(0.07)
H13CN (2–1) 3.42(0.56) 1.06 11.1(1.8)−25.1(3.9)

B1b
DCN (2–1) 0.27(0.05) 1.13 1.5(0.2)−4.1(0.5) 0.48(0.12)−0.56(0.15)
H13CN (2–1) 1.29(0.28) 0.88 4.2(1.1)−9.5(2.4)

Total
DCN (2–1) 0.44(0.07) 1.15 1.7(0.3)−4.5(0.7) 0.32(0.07)−0.37(0.09)
H13CN (2–1) 2.11(0.37) 1.04 6.8(1.2)−15.5(2.8)

Notes.

(a)

Uncertainties are reported in parentheses and include the statistical error and the uncertainty in the flux calibration.

(b)

Dfrac(HCN) = N(DCN)/N(HCN) computed using 12C/13C = 77 (Wilson & Rood 1994) to obtain N(HCN) from N(H13CN).

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