S. Takano et al., OBSERVATIONS OF C-13 ISOTOPOMERS OF HC3N AND HC5N IN TMC-1 - EVIDENCEFOR ISOTOPIC FRACTIONATION, Astronomy and astrophysics, 329(3), 1998, pp. 1156-1169
The C-13 substitutions of HC3N ((HCCCN)-C-13, (HCCCN)-C-13, and (HCCCN
)-C-13) were observed in TMC-1 using the J = 2 - 1, 4 - 3, and 5 - 4 r
otational transitions at 18, 36, and 45 GHz, respectively. The spectra
l lines of (HCCCN)-C-13 are stronger than those of (HCICCN)-C-13 in al
l observed transitions, while the spectral lines of (HCCCN)-C-13 and (
HCCCN)-C-13 show similar intensity. These differences in the intensiti
es are most probably due to C-13 isotopic fractionation in the formati
on process of HC3N. The abundance ratios are 1.0:1.0:1.4 for [(HCCCN)-
C-13] : [(HCCCN)-C-13] : [(HCCCN)-C-13] at the cyanopolyyne peak in TM
C-1: the C-13 isotope is concentrated in a carbon atom adjacent to the
nitrogen atom. Based on these observational results, the production m
echanism of HC3N was discussed. As a result, the formation reactions b
etween a hydrocarbon molecule with two carbon atoms (e.g. C2H2) and a
molecule with a C-13 enriched CN group can explain C-13 isotopic fract
ionation: a neutral-neutral reaction between C2H2 and CN is probably m
ost important. The ratio of the contributions of two types of the HC3N
formation reactions which can and cannot produce C-13 isotopic fracti
onation is discussed. In addition, the C-13 isotopic species of HC5N (
(HCCCCCN)-C-13 and (HCCCCCN)-C-13) were also observed at the cyanopoly
yne peak in TMC-1 using the J = 9 - 8 rotational transitions at 23.7 G
Hz. The intensity of (HCCCCCN)-C-13 is marginally stronger than that o
f HC13 CCCCN. Furthermore, the (J, K) = (2, 2) emission of NH3 was sim
ultaneously observed with the C-13 isotopic species of HC5N. With the
additional observation of the (J, K) = (1,1) emission of NH3, the rota
tional temperature between the (1,1) and (2,2) levels, and the column
density of NH3 are determined for the cyanopolyyne peak in TMC-1.