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Table 13:

Parameters of our best-fit LTE models of methyl cyanide, ethyl cyanide, vinyl cyanide, and aminoacetonitrile, and column density upper limit for cyanomethylidyne.
Moleculea Sizeb $T_{\rm rot}$c Nd $\Delta V^{e}$ $V_{{\rm off}}$f
  ('') (K) (cm-2) (km s-1) (km s-1)
(1) (2) (3) (4) (5) (6)
CH3CN 2.7 200 $ 2.00 \times 10^{18}$ 6.5 -1.0
  2.7 200 $ 8.00 \times 10^{17}$ 6.5 9.0
  2.7 200 $ 1.00 \times 10^{17}$ 8.0 -11.0
C2H5CN 3.0 170 $ 1.20 \times 10^{18}$ 6.5 -1.0
  2.3 170 $ 1.40 \times 10^{18}$ 6.5 9.0
  1.7 170 $ 9.00 \times 10^{17}$ 8.0 -11.0
C2H3CN 2.3 170 $ 8.00 \times 10^{17}$ 7.0 -1.0
  2.3 170 $ 2.40 \times 10^{17}$ 7.0 9.0
  2.3 170 $ 1.00 \times 10^{17}$ 10.0 -9.0
NH2CH2CN 2.0 100 $ 2.80 \times 10^{16}$ 7.0 0.0
CCNg 3.0 200 < $1.20 \times 10^{17}$ 6.5 -1.0
  3.0 200 < $1.20 \times 10^{17}$ 6.5 9.0
Notes: a We used the JPL entry for CH3CN (version 3), and the CDMS entries for C2H5CN (ver. 1), C2H3CN (ver. 1), NH2CH2CN (ver. 1), and CCN (ver. 1). See references to the laboratory data therein. b Source diameter (FWHM). c Temperature. d Column density. e Linewidth (FWHM). f Velocity offset with respect to the systemic velocity of Sgr B2(N) $V_{{\rm lsr}} = 64$ km s-1. g The column density upper limit is $\sim$$3\sigma$. The other parameters were fixed.

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