J/A+A/591/A75    Millimeter wave spectrum of methyl cyanate (Kolesnikova+, 2016)

The millimeter wave spectrum of methyl cyanate: a laboratory study and astronomical search in space. Kolesnikova L., Alonso J.L., Bermudez C., Alonso E.R., Tercero B., Cernicharo J., Guillemin J.-C. <Astron. Astrophys. 591, A75 (2016)> =2016A&A...591A..75K 2016A&A...591A..75K (SIMBAD/NED BibCode)
ADC_Keywords: Interstellar medium ; Spectroscopy ; Atomic physics Keywords: astrochemistry - line: identification - techniques: spectroscopic - astronomical databases: miscellaneous - molecular data Abstract: The recent discovery of methyl isocyanate (CH3NCO) in Sgr B2(N) and Orion KL makes methyl cyanate (CH3OCN) a potential molecule in the interstellar medium. The aim of this work is to fulfill the first requirement for its unequivocal identification in space, i.e. the availability of transition frequencies with high accuracy. The room-temperature rotational spectrum of methyl cyanate was recorded in the millimeter wave domain from 130 to 350GHz. All rotational transitions revealed A-E splitting owing to methyl internal rotation and were globally analyzed using the ERHAM program. The data set for the ground torsional state of methyl cyanate exceeds 700 transitions within J"=10-35 and K"a=0-13 and newly derived spectroscopic constants reproduce the spectrum close to the experimental uncertainty. Spectral features of methyl cyanate were then searched for in Orion KL, Sgr B2(N), B1-b, and TMC-1 molecular clouds. Upper limits to the column density of methyl cyanate are provided. Description: Observed and predicted rotational transition frequencies of methyl cyanate in the ground torsional state. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tables1.dat 39 738 Observed rotational transition frequencies of methyl cyanate in the ground torsional state tables2.dat 62 1962 Predicted rotational transition frequencies of methyl cyanate in the ground torsional state -------------------------------------------------------------------------------- Byte-by-byte Description of file: tables1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1 I1 --- Sigma [0/1] Symmetry number (1) 3- 4 I2 --- J1 Upper state J quantum number (J') 6- 7 I2 --- Ka1 Upper state Ka quantum number (Ka') 9- 10 I2 --- Kc1 Upper state Kc quantum number (Kc') 12- 13 I2 --- J0 Lower state J quantum number (J") 15- 16 I2 --- Ka0 Lower state Ka quantum number (Ka") 18- 19 I2 --- Kc0 Lower state Kc quantum number (Kc") 21- 30 F10.3 MHz FreqObs Observed transition frequency 32- 37 F6.3 MHz O-C Observed minus calculated frequency 39 A1 --- Comment Comment (2) -------------------------------------------------------------------------------- Note (1): The symmetry numbers sigma = 0 and 1 label the A and E transitions, respectively. Note (2): Blended transitions are indicated using the capital letter B. In case of the lines composed from degenerate asymmetric rotor transitions, equal weights were assigned to the components of such blends. Any other transitions blended accidentally, as those corresponding to not related A and E components, were not included in the fit. The capital letter E indicates the excluded transitions. -------------------------------------------------------------------------------- Byte-by-byte Description of file: tables2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1 I1 --- Sigma [0/1] Symmetry number (1) 3- 4 I2 --- J1 Upper state J quantum number (J') 6- 7 I2 --- Ka1 Upper state Ka quantum number (Ka') 9- 10 I2 --- Kc1 Upper state Kc quantum number (Kc') 12- 13 I2 --- J0 Lower state J quantum number (J") 15- 16 I2 --- Ka0 Lower state Ka quantum number (Ka") 18- 19 I2 --- Kc0 Lower state Kc quantum number (Kc") 21- 30 F10.3 MHz FreqPred Predicted frequency 32- 36 F5.3 MHz e_FreqPred Uncertainty of the predicted frequency (2) 38- 46 F9.5 D+2 Smu2 Intensity (3) 48- 54 F7.3 cm-1 E1 Upper level energy (E') (4) 56- 62 F7.3 cm-1 E0 Lower level energy (E") -------------------------------------------------------------------------------- Note (1): The symmetry numbers sigma = 0 and 1 label the A and E transitions, respectively. Note (2): Only transitions with uncertainty <1MHz are included. Note (3): Given in terms of calculated line strengths multiplied by the square of the corresponding dipole moment component. Note (4): The upper state energies refer to a hypothetical unsplit J=0 energy level. -------------------------------------------------------------------------------- Acknowledgements: Lucie Kolesnikova, lucie.kolesnikova(at)uva.es
(End) Lucie Kolesnikova [GEM, UVa, Spain], Patricia Vannier [CDS] 04-May-2016
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