Table B.1
Sorted list by frequency of the transitions used in the MADCUBA pixel-by-pixel method (Fig. 10).
| Frequency (GHz) | Species | Transition | logI (nm2 MHz) | EUP (K) | τ(×10−2) |
|---|---|---|---|---|---|
| 217.272 | CH2(OH)CHO | 314,27,0 → 313,28,0 | −3.7 | 290 | 1.3 ± 1.4 |
| 217.604 | CH2(OH)CHO | 245,19,0 → 236,18,0 | −3.9 | 187 | 1.1 ± 1.4 |
| 217.626 | CH2(OH)CHO | 95,5,0 → 84,4,0 | −3.7 | 40 | 3.3 ± 1.5 |
| 217.831 | CH2(OH)CHO | 95,4,0 → 84,5,0 | −3.7 | 40 | 3.3 ± 1.5 |
| 218.261 | CH2(OH)CHO | 203,17,0 → 194,16,0 | −3.6 | 126 | 3.0 ± 1.5 |
| 219.123 | CH2(OH)CHO | 293,26,0 → 292,27,0 | −3.7 | 250 | 1.3 ± 1.4 |
| 220.055 | CH2(OH)CHO | 3510,26,0 → 359,27,0 | −3.6 | 410 | 0.9 ± 1.4 |
| 220.464 | CH2(OH)CHO | 202,18,0 → 193,17,0 | −3.4 | 120 | 4.8 ± 1.6 |
| 217.140 | aGg’-(CH2OH)2 | 214,17,0 → 204,16,1 | −3.6 | 124 | 0.0193 |
| 217.450 | aGg’-(CH2OH)2 | 241,24,0 → 231,23,1 | −3.6 | 136 | 0.0196 |
| 217.450 | aGg’-(CH2OH)2 | 240,24,0 → 230,23,1 | −3.7 | 136 | 0.0152 |
| 217.588 | aGg’-(CH2OH)2 | 212,19,1 → 202,18,0 | −3.7 | 117 | 0.0178 |
| 218.706 | aGg’-(CH2OH)2 | 2212,11,0 → 2112,10,1 | −3.8 | 195 | 6.2 × 10−3 |
| 218.706 | aGg’-(CH2OH)2 | 2212,10,0 → 2112,9,1 | −4.0 | 195 | 4.8 × 10−3 |
| 219.090 | aGg’-(CH2OH)2 | 2210,13,0 → 2110,12,1 | −3.8 | 174 | 9.1 × 10−3 |
| 219.385 | aGg’-(CH2OH)2 | 2611,16,1 → 2610,16,0 | −5.5 | 230 | 1.05 × 10−4 |
| 219.385 | aGg’-(CH2OH)2 | 229,14,0 → 219,13,1 | −3.7 | 164 | 0.0107 |
| 219.385 | aGg’-(CH2OH)2 | 2611,15,1 → 2610,17,0 | −5.4 | 230 | 1.35 × 10−4 |
| 219.385 | aGg’-(CH2OH)2 | 229,13,0 → 219,12,1 | −3.8 | 164 | 8.3 × 10−3 |
| 219.386 | aGg’-(CH2OH)2 | 4512,34,1 → 4413,31,1 | −5.4 | 580 | 5.3 × 10−6 |
| 219.581 | aGg’-(CH2OH)2 | 221,21,1 → 211,20,0 | −3.6 | 122 | 0.021 |
| 219.765 | aGg’-(CH2OH)2 | 204,16,1 → 194,15,0 | −3.6 | 114 | 0.021 |
| 220.497 | aGg’-(CH2OH)2 | 227,15,0 → 217,14,1 | −3.8 | 149 | 0.0109 |
Notes. Frequency shows the rest frequency of the transitions in GHz; Transition shows the 
where J is the total angular momentum and Ka and Kc are the projections of J onto the a and c inertial axis; log I is the logarithm of the line intensity in nm2 MHz; Eup is the energy of higher level in K, and τ is the optical depth of the transitions.
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