J/A+A/493/565     Deuterated and 15N ethyl cyanides         (Margules+, 2009)

Rotational spectrum of deuterated and 15N ethyl cyanides: CH3CHDCN, CH2DCH2CN and CH3CH2C15N. Margules L., Motiyenko R., Demyk K., Tercero B., Cernicharo J., Sheng M., Wiedmann M., Gripp J., Maeder H., Demaison J. <Astron. Astrophys. 493, 565 (2009)> =2009A&A...493..565M 2009A&A...493..565M
ADC_Keywords: Atomic physics Keywords: line: identification - methods: laboratory - molecular data - ISM: molecules - radio lines: ISM - submillimeter Abstract: Ethyl cyanide is an abundant molecule in hot molecular clouds. Its rotational spectrum is very dense and several hundreds of rotational transitions within the ground state have been identified in molecular clouds in the 40-900GHz frequency range. Lines from 13C isotopically substituted ethyl cyanide have been recently identified in Orion. To enable the search and the possible detection of other isotopologues of ethyl cyanide in interstellar objects we have studied the rotational spectrum of deuterated ethyl cyanide: CH2DCH2CN (in-plane and out-of-plane) and CH3CHDCN and the spectrum of 15N substituted ethyl cyanide CH2DCH2C15N. The rotational spectrum of these species in the ground state was measured in the microwave and millimeter-submillimeter wavelength range using waveguide Fourier transform spectrometers (4-40GHz) and a source-modulated spectrometer employing backward-wave oscillators (BWOs) (150-260 and 580-660GHz). More than 300 lines were identified for each species for J values up to 71-80 and Ka values up to 28-31 depending on the isotopologues. The experimental spectra were analysed using a Watson's Hamiltonian using A-reduction in Ir representation. From the fitting procedure, accurate spectroscopic constants were derived for each species. These new sets of spectroscopic constants enable us to compute reliable prediction of the rotational spectrum (lines frequency and intensity) in the 4-1000GHz frequency range and for J and Ka up to 80 and 31, respectively. This experimental study allowed us to detect for the first time 15N substituted ethyl cyanide CH2DCH2C15N in Orion. The derived column density and rotational temperature are 1013cm-2 and 150K for the plateau and 3x1014cm-2 and 300K for the hot core. The deuterated species were search for but are not detected. The upper limit on the column density of each deuterated isotopologues is 1014cm-2. Description: The tables present the predicted line-center frequency and line strength of rotational transitions for the 15N-isotopologue of ethyl cyanide (CH3CH2C15N) and of its deuterated isotopologues: CH3CHDCN, CH2DCH2CN in-plane and out-of-plane, up to 1THz and for J<100. The frequencies are calculated using a Watson's Hamiltonian in A-reduction in Ir representation. The error on the frequency given in the tables is the standard deviation. To get a more realistic estimation of the error it must be multiplied by a factor 3, for the strongest lines to 10, for the weakest lines. However, the general trend is that for the lines that are the most suitable for interstellar detection, i.e. the strongest lines having J value up to ∼50 and a low Ka value, the error on the predicted frequencies is a few hundred kHz, suitable for line identification in the interstellar spectra. The error is larger for the weakest lines and increases as J and Ka become larger, i.e., as the frequency increases. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table7.dat 50 13475 Predicted transitions of CH3CH2C15N table8.dat 50 14292 Predicted transitions of CH3CHDCN table9.dat 50 13610 Predicted transitions of CH2DCH2CN-in-plane table10.dat 50 14234 Predicted transitions of CH2DCH2CN-out-of-plane -------------------------------------------------------------------------------- See also: J/A+A/466/255 : Isotopic ethyl cyanide (Demyk+, 2007) Byte-by-byte Description of file: table*.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 3 I3 --- J0 J value of the lower state 5- 6 I2 --- Ka0 Ka value of the lower state 8- 10 I3 --- Kc0 Kc value of the lower state 12- 13 I2 --- J1 J value of the upper state 15- 16 I2 --- Ka1 Ka value of the upper state 18- 19 I2 --- Kc1 Kc value of the upper state 21- 29 F9.2 MHz Freq Calculated frequency 31- 34 F4.2 MHz e_Freq Error on the calculated frequency 36- 40 F5.2 --- S Line strength 42 A1 --- Dipole [A/B] Type of the transition 44- 50 F7.2 cm-1 E0 Energy of the lower state -------------------------------------------------------------------------------- Acknowledgements: Karine Demyk, demyk(at)cesr.fr
(End) Patricia Vannier [CDS] 24-Nov-2008
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