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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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