Table E.1
Rotational temperatures derived from population diagrams of selected (complex) organic molecules toward CALYPSO sources.
| Molecule | States(a) | Npop (b) | Tfit (c) | |
|---|---|---|---|---|
| (K) | ||||
| L1448-2A | ||||
| CH3OH | v = 0 | 8 | 160 | (108) |
| L1448-2Ab | ||||
| CH3OH | v = 0 | 10 | 970 | (3508) |
| HNCO | v = 0 | 2 | – | |
| L1448-C | ||||
| CH3OH | v = 0, vt = 1 | 13 | 107 | (11) |
| CH3OCH3 | v = 0 | 3 | 75 | (5) |
| CH3OCHO | v = 0 | 7 | 39 | (27) |
| CH3CHO | v = 0 | 13 | 77 | (21) |
| NH2CHO | v = 0 | 2 | – | |
| CH3CN | v = 0 | 4 | 105 | (23) |
| HNCO | v = 0 | 3 | 59 | (3) |
| IRAS2A1 | ||||
| CH3OH | v = 0, vt = 1 | 24 | 229 | (21) |
| C2H5 OH | v = 0 | 17 | 703 | (890) |
| CH3OCH3 | v = 0 | 6 | 113 | (9) |
| CH3OCHO | v = 0, vt = 1 | 19 | 128 | (16) |
| CH3CHO | v = 0, v = 1 | 17 | 161 | (36) |
| NH2CHO | v = 0, v12 = 1 | 4 | 404 | (163) |
| CH3CN | v = 0, v8 = 1 | 5 | 161 | (17) |
| (CH2OH)2 | v = 0 | 20 | 173 | (86) |
| HNCO | v = 0 | 5 | 254 | (22) |
| NH2CN | v = 0 | 7 | 200 | (108) |
| SVS13A | ||||
| CH3OH | v = 0, vt = 1 | 23 | 285 | (82) |
| C2H5 OH | v = 0 | 26 | 274 | (115) |
| CH3OCH3 | v = 0, v11 = 1 | 9 | 94 | (7) |
| CH3OCHO | v = 0, vt = 1,vt = 2 | 28 | 109 | (12) |
| CH3CHO | v = 0, v = 1 | 26 | 113 | (14) |
| NH2CHO | v = 0, v12 = 1 | 4 | 351 | (117) |
| CH3CN | v = 0, v8 = 1 | 6 | 222 | (49) |
| C2H5 CN | v = 0 | 6 | 33 | (16) |
| (CH2OH)2 | v = 0 | 24 | 98 | (19) |
| CH2 (OH)CHO | v = 0 | 7 | 106 | (24) |
| HNCO | v = 0 | 5 | 233 | (17) |
| NH2CN | v = 0 | 8 | 317 | (136) |
| IRAS4A2 | ||||
| CH3OH | v = 0, vt = 1 | 24 | 307 | (56) |
| C2H5 OH | v = 0 | 25 | 127 | (33) |
| CH3OCH3 | v = 0, v11 = 1, v15 = 1 | 10 | 134 | (6) |
| CH3OCHO | v = 0, vt = 1, vt = 2 | 34 | 150 | (11) |
| CH3CHO | v = 0, v = 1, v = 2 | 54 | 220 | (18) |
| NH2CHO | v = 0, v12 = 1 | 4 | 536 | (239) |
| CH3CN | v = 0 | 5 | 142 | (13) |
| C2H5 CN | v = 0 | 6 | – | |
| (CH2OH)2 | v = 0 | 28 | 126 | (47) |
| CH2 (OH)CHO | v = 0 | 15 | 196 | (67) |
| HNCO | v = 0 | 5 | 280 | (56) |
| NH2CN | v = 0 | 10 | 280 | (171) |
| IRAS4B | ||||
| CH3OH | v = 0, vt = 1 | 18 | 305 | (52) |
| C2H5 OH | v = 0 | 12 | 238 | (123) |
| CH3OCH3 | v = 0 | 3 | 95 | (28) |
| CH3OCHO | v = 0, vt = 1 | 14 | 328 | (110) |
| CH3CHO | v = 0, v = 1, v = 2 | 46 | 318 | (53) |
| NH2CHO | v = 0 | 2 | – | |
| CH3CN | v = 0 | 3 | – | |
| C2H5 CN | v = 0 | 4 | 14 | (6) |
| CH2 (OH)CHO | v = 0 | 8 | 180 | (74) |
| HNCO | v = 0 | 6 | 379 | (62) |
| SerpM-S68N | ||||
| CH3OH | v = 0, vt = 1 | 9 | 210 | (37) |
| CH3OCHO | v = 0 | 7 | 10 | (3) |
| CH3CN | v = 0 | 3 | – | |
| SerpM-SMM4b | ||||
| CH3OH | v = 0, vt = 1 | 16 | 223 | (46) |
| HNCO | v = 0 | 3 | 383 | (267) |
| SerpS-MM18a | ||||
| CH3OH | v = 0, vt = 1 | 18 | 154 | (22) |
| C2H5 OH | v = 0 | 9 | 238 | (202) |
| CH3OCH3 | v = 0 | 4 | 106 | (15) |
| CH3OCHO | v = 0, vt = 1 | 9 | 171 | (65) |
| CH3CHO | v = 0 | 12 | 78 | (41) |
| NH2CHO | v = 0 | 2 | 80 | (41) |
| CH3CN | v = 0, v8 = 1 | 6 | 244 | (28) |
| C2H5 CN | v = 0 | 6 | 33 | (12) |
| HNCO | v = 0 | 5 | 178 | (25) |
| SerpS-MM18b | ||||
| CH3OH | v = 0 | 5 | 69 | (10) |
| CH3CN | v = 0 | 2 | 17 | (18) |
| HNCO | v = 0 | 2 | 12 | (28) |
| L1157 | ||||
| CH3OH | v = 0 | 11 | 199 | (50) |
| CH3OCHO | v = 0 | 2 | 8 | (4) |
| CH3CN | v = 0 | 3 | 274 | (536) |
Notes. (a) Vibrational or torsional states that were taken into account to fit the population diagram. (b) Number of detected lines displayed in the population diagram and used to fit the rotational temperature. (c) The standard deviation of the fit is given in parentheses. These uncertainties are purely statistical and should be viewed with caution. They may be underestimated. Rotational temperatures with a signal-to-noise ratio higher than 3.5 are indicated in bold face. Negative temperatures or temperatures above 1500 K, likely the result of high uncertainties or line contamination by unidentified species, are not shown and are replaced with a dash.
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