Open Access
Table A.5
Line intensities from IRAM observations.
Date | Molecule | Transition | Frequency(a) | Beam | Offset(b) | Intensity | Doppler shift |
---|---|---|---|---|---|---|---|
(yyyy/mm/dd.dd) | (MHz) | (′′) | (′′) | (K km s−1) | (km s−1) | ||
64P/Swift-Gehrels | |||||||
2018/12/11.75 | HCN | 3–2 | 265 886.434 | 9.3 | 2.9 | 0.349 ± 0.035 | −0.225 ± 0.063 |
2018/12/17.95 | CH3CN | 14–11 (4 lines) | 257 527–257 448 | 9.5 | 2.4 | (sum) < 0.147 | |
2018/12/11.75 | CH3OH | J3 − J2A± (8 l.) | 251 738–251 924 | 9.7 | 2.9 | sum = 0.158 ± 0.048 | −0.12 ± 0.14 |
CH3OH | 110 − 101 A+ | 250 507.016 | 0.008 ± 0.020 | ||||
CH3OH | 20 − 1−1 E | 254 015.377 | 9.6 | 0.012 ± 0.019 | |||
CH3OH | 52 − 41 E | 266 838.123 | 9.3 | 0.074 ± 0.022 | −0.14 ± 0.13 | ||
2018/12/17.95 | CH3OH | 50 − 40E | 241 700.168 | 10.0 | 2.4 | 0.053 ± 0.021 | + 0.04 ± 0.21 |
5−1 − 4−1E | 241 767.247 | 0.062 ± 0.020 | −0.27 ± 0.17 | ||||
50 − 40 A | 241 791.367 | 0.124 ± 0.021 | −0.17 ± 0.09 | ||||
51 − 41E | 241 879.038 | 0.048 ± 0.021 | + 0.03 ± 0.23 | ||||
5± 2 − 4± 2E | 241 904.401 | 0.045 ± 0.021 | −0.22 ± 0.28 | ||||
51 − 41 A− | 243 915.811 | 0.034 ± 0.024 | −0.44 ± 0.50 | ||||
CH3OH | 21 − 10E | 261 805.736 | 0.058 ± 0.025 | −0.11 ± 0.20 | |||
2018/12/17.95 | CS | 5–4 | 244 935.557 | 9.9 | 2.4 | 0.062 ± 0.022 | −0.12 ± 0.19 |
2018/12/17.95 | SO | 6.6–5.5 | 258 255.826 | 9.5 | 2.4 | 0.025 ± 0.022 | |
6.7–5.6 | 261 843.721 | 9.4 | −0.058 ± 0.025 | ||||
2018/12/17.95 | HNCO | 110,11 − 100,10 | 241 774.032 | 10.0 | 2.4 | 0.003 ± 0.021 | |
38P/Stephan-Oterma | |||||||
2018/12/13.12 | CH3CN | 8–7 (4 lines) | 147 175–147 149 | 16.7 | 2.2 | (sum) < 0.162 | |
2018/12/13.12 | CH3CN | 9–8 (4 lines) | 165 569–165 540 | 14.9 | 2.2 | (sum) < 0.195 | |
2018/12/17.93 | CH3CN | 14–11 (4 lines) | 257 527–257 448 | 9.5 | 2.2 | (sum) < 0.386 | |
2018/12/13.12 | CS | 3–2 | 146 969.029 | 16.7 | 2.2 | <0.075 | |
2018/12/17.93 | CS | 5–4 | 244 935.557 | 9.9 | 3.1 | <0.136 | |
2018/12/12/12 | CH3OH | 8−1 − 70E | 229 758.811 | 10.6 | 2.2 | <0.147 | |
2018/12/13.12 | CH3OH | J1 − J0E (6 lines) | 165 050–166 678 | 14.9 | 2.2 | (sum) < 0.242 | |
CH3OH | 32 − 21E | 170 060.581 | 14.6 | <0.140 | |||
2018/12/17.93 | CH3OH | 50 − 40E | 241 700.168 | 10.0 | 3.1 | 0.012 ± 0.044 | |
5−1 − 4−1E | 241 767.247 | 0.099 ± 0.043 | + 0.14 ± 0.22 | ||||
50 − 40 A | 241 791.367 | 0.089 ± 0.039 | + 0.18 ± 0.20 | ||||
51 − 41 E | 241 879.038 | 0.028 ± 0.045 | |||||
5± 2 − 4± 2 E | 241 904.401 | 0.051 ± 0.044 | −0.23 ± 0.47 | ||||
51 − 41 A− | 243 915.811 | 0.038 ± 0.047 | |||||
CH3 OH | 21 − 10 E | 261 805.736 | 9.4 | <0.157 | |||
2018/12/12.12 | H2 CO | 31,3 − 21,2 | 211 211.469 | 11.4 | 2.2 | <0.109 | |
H2 CO | 31,2 − 21,1 | 225 697.772 | 10.7 | <0.132 | |||
2018/12/13.12 | H2 CO | 21,1 − 11,0 | 150 498.334 | 16.3 | 2.2 | <0.128 | |
2018/12/12.12 | CO | 2–1 | 230 538.000 | 10.5 | 2.2 | <0.117 | |
2018/12/13.12 | H2 S | 11,0 − 10,1 | 168 762.762 | 14.7 | 2.2 | <0.125 |
Notes. (a)From Müller et al. (2005) and Pickett et al. (1998). (b)Half power Gaussian beam width and average radial pointing offset. On average 9.3–10.0′′ corresponded to 4000–4400 km at the distance of comet 64P and 9.4–16.7′′ corresponded to 5200–9300 km at the distance of 38P.
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