Molecule | Transition | Frequency |
![]() |
Peak position (mpc)(d) |
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|||||||||
(MHz) | (K) | NE slice | SW slice | model | (K km s-1) | n=105 cm-3 | LTE | ||||||||
C2H | NJ | = | 47/2 | ![]() |
349400.5(a) | 42 | -14 | ![]() |
-23 | ![]() |
-16 | 10.2 | ![]() |
5.5 ![]() |
2.7 ![]() |
C2H | NJ | = | 49/2 | ![]() |
349337.8(b) | 42 | -14 | ![]() |
-23 | ![]() |
-16 | 13.5 | ![]() |
6.4 ![]() |
2.9 ![]() |
o-H2CO | JKpKo | = | 515 | ![]() |
351768.6 | 62 | -3 | ![]() |
-7 | ![]() |
-12 | 11.1 | ![]() |
9.7 ![]() |
4.3 ![]() |
SO | NJ | = | 89 | ![]() |
346528.5 | 79 | -2 | ![]() |
-5 | ![]() |
8 | 6.1 | ![]() |
1.5 ![]() |
7.7 ![]() |
C18O | J | = | 2 | ![]() |
219560.4 | 16 | 0 | ![]() |
0 | ![]() |
0 | 95.2 | ![]() |
1.5 ![]() |
1.8 ![]() |
HCN | J | = | 3 | ![]() |
265886.2(c) | 26 | 3 | ![]() |
-1 | ![]() |
8 | 420 | ![]() |
8.1 ![]() |
4.4 ![]() |
13CO | J | = | 3 | ![]() |
330588.0 | 32 | 4 | ![]() |
-1 | ![]() |
2 | 132 | ![]() |
>2.1 ![]() |
>2.5 ![]() |
(a) Blend of F=4-3 and F=3-2 hyperfine components (separation 1.4 MHz). (b) Blend of F=5-4 and F=4-3 hyperfine components (separation 1.3 MHz). (c) Blend of F=3-3, F=3-2 and F=2-1 hyperfine components (total separation 1.5 MHz). (d) Fitted position of the emission peak along the slice through the northeast and southwest cores (see Fig. 1), and the modeled slice (Fig. 3, bottom panel), all relative to the C18O peak. (e) Fitted value of integrated intensity at peak position along the northeast slice (see Fig. 1); uncertainties include fitting uncertainty and 15% absolute calibration uncertainty. (f) Column density uncertain due to high optical depth; values listed here are lower limits. (g) Beam-averaged column densities for n=105 cm-3 and in LTE, both at T=85 K. |
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