J/A+A/636/A33    Glutaronitrile rotational spectroscopy         (Cabezas+, 2020)

Rotational spectroscopy and astronomical search of glutaronitrile. Cabezas C., Bermudez C., Endo Y., Tercero B., Cernicharo J. <Astron. Astrophys. 636, A33 (2020)> =2020A&A...636A..33C 2020A&A...636A..33C (SIMBAD/NED BibCode)
ADC_Keywords: Atomic physics Keywords: ISM: molecules - methods: laboratory: molecular - molecular data - line: identification Abstract: Nitriles constitute almost 15% of the molecules observed in the interstellar medium (ISM), surprisingly only two dinitriles have been detected in the ISM so far. The lack of astronomical detections for dinitriles may be partly explained by the absence of laboratory rotational spectroscopic data. Our goal is the investigation of the rotational spectrum of glutaronitrile, NC-CH2-CH2-CH2-CN, in order to allow its possible detection in the ISM. The rotational spectra of glutaronitrile was measured using two different experimental setups. A Fourier transform microwave spectrometer was employed to observe the supersonic jet rotational spectrum of glutaronitrile between 6 and 20GHz. In addition the mmW spectrum was observed in the frequency range 72-116.5GHz using a broadband millimeter-wave spectrometer based on radio astronomy receivers with fast Fourier transform backends. The spectral searches were supported by high-level ab initio calculations. A total of 111 rotational transitions with maximum values of J and Ka quantum numbers 54 and 18, respectively, were measured for the gg conformer of glutaronitrile. The analysis allowed us to accurately determine the rotational, nuclear quadrupole coupling, quartic and sextic centrifugal distortion constants. These rotational parameters were employed to search for glutaronitrile in the cold and warm molecular clouds Orion KL, Sgr B2(N), B1-b and TMC-1, using the spectral surveys captured by IRAM 30m at 3mm. Glutaronitrile was not detected and the upper limits column densities are derived. Those are a factor of 1.5 and 5 lower than those obtained for the total column densities of the analogous succionitrile in Orion KL and Sgr B2, respectively. Description: The rotational investigation of a larger dinitrile, glutaronitrile, with one more atomic carbon in the hydrocarbon skeleton than succinonitrile is reported. To record the rotational spectrum of glutaronitrile, two different spectroscopic techniques have been employed; a high resolution Fourier transform microwave (FTMW) pulsed supersonic jet spectrometer operating in the centimetre wave region and a broadband millimetre-wave spectrometer based on radio astronomy receivers with fast Fourier transform backends. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tablea1.dat 62 228 Measured rotational transitions for glutaronitrile observed by FTMW spectroscopy tablea2.dat 65 89 Measured rotational transitions for glutaronitrile observed in the mmW region tablea3.dat 47 16239 Predicted transition frequencies for glutaronitrile up to 300GHz -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 2 I1 --- J' Quantum number J for upper level 5 I1 --- Ka' Quantum number Ka for upper level 8 I1 --- Kc' Quantum number Kc for upper level 11 I1 --- I' Quantum number I for upper level 14 I1 --- F' Quantum number F for upper level 17 I1 --- J" Quantum number J for lower level 20 I1 --- Ka" Quantum number Ka for lower level 23 I1 --- Kc" Quantum number Kc for lower level 26 I1 --- I" Quantum number I for lower level 29 I1 --- F" Quantum number F for lower level 35- 43 F9.3 MHz Freq Measured frequency 48- 53 F6.3 MHz O-C Difference between observed & calculated freq. 58- 62 F5.3 MHz Uncert Uncertainty associated to frequency -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 3- 4 I2 --- J' Quantum number J for upper level 7- 8 I2 --- Ka' Quantum number Ka for upper level 11- 12 I2 --- Kc' Quantum number Kc for upper level 17- 18 I2 --- J" Quantum number J for lower level 21- 22 I2 --- Ka" Quantum number Ka for lower level 25- 26 I2 --- Kc" Quantum number Kc for lower level 31- 41 F11.4 MHz Freq Measured frequency 47- 52 F6.3 MHz O-C Difference between observed & calculated freq. 61- 65 F5.3 MHz Uncert Uncertainty associated to frequency -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea3.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 2- 3 I2 --- J' Quantum number J for upper level 6- 7 I2 --- Ka' Quantum number Ka for upper level 10- 11 I2 --- Kc' Quantum number Kc for upper level 14- 15 I2 --- J" Quantum number J for lower level 18- 19 I2 --- Ka" Quantum number Ka for lower level 22- 23 I2 --- Kc" Quantum number Kc for lower level 27- 37 F11.4 MHz Freq Frequency 41- 47 F7.4 [nm2/MHz] logInt Base 10 logarithm of the integrated intensity -------------------------------------------------------------------------------- Acknowledgements: Carlos Cabezas, carlos.cabezas(at)csic.es
(End) Patricia Vannier [CDS] 04-Mar-2020
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