Table 1
CH3CN transitions analyzed in this paper.
Transition | Frequency (GHz) | Elower (K) |
---|---|---|
Main isotopologue, ground state | ||
120−110 | 220.747261 | 57.87 |
121−111 | 220.743011 | 64.96 |
122−112 | 220.730261 | 86.25 |
123−113 | 220.709017 | 121.71 |
124−114 | 220.679287 | 171.36 |
125−115 | 220.641084 | 235.17 |
126−116 | 220.594423 | 313.13 |
130−120 | 239.137916 | 68.39 |
131−121 | 239.133313 | 75.48 |
132−122 | 239.119504 | 96.77 |
133−123 | 239.096497 | 132.23 |
134−124 | 239.064299 | 181.88 |
135−125 | 239.022924 | 245.68 |
136−126 | 238.972390 | 323.64 |
137−127 | 238.912715 | 415.73 |
138−128 | 238.843926 | 521.93 |
139−129 | 238.766049 | 642.21 |
140−130 | 257.527384 | 79.79 |
141−131 | 257.522428 | 86.88 |
142−132 | 257.507561 | 108.16 |
143−133 | 257.482792 | 143.63 |
144−134 | 257.448128 | 193.27 |
145−135 | 257.403584 | 257.07 |
146−136 | 257.349179 | 335.03 |
147−137 | 257.284935 | 427.11 |
148−138 | 257.210877 | 533.31 |
149−139 | 257.127035 | 653.59 |
Vibrationally excited v8 = 1 | ||
121−11−1 | 221.625828 | 577.13 |
13CH3CN isotopologue, ground state | ||
130−120 | 232.234188 | 66.38 |
131−121 | 232.229822 | 73.48 |
132−122 | 232.216726 | 94.79 |
133−123 | 232.194906 | 130.30 |
134−124 | 232.164369 | 180.01 |
135 − 125 | 232.125130 | 243.89 |
136 − 126 | 232.077203 | 321.94 |
137 − 127 | 232.020609 | 414.15 |
Notes. Parameters of the transitions obtained from the molecular databases CDMS (Müller et al. 2005; Endres et al. 2016) and JPL (Pickett et al. 1998). In more detail, the CH3CN and 13CH3 CN entries are based on Müller et al. (2015, 2009), respectively, with important additional data especially from Cazzoli & Puzzarini (2006) and Pearson & Müller (1996). The dipole moment of CH3 CN used to derive the Einstein Aul values is taken from Gadhi et al. (1995); the dipole moment of 13CH3CN is assumed to agree with that of the main isotopologue, as is frequently done.
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