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MICROWAVE AND FIR SPECTROSCOPY OF DIMETHYLSULFIDE IN THE GROUND, FIRST AND SECOND EXCITED TORSIONAL STATES V. Ilyushin1, I. Armieieva1, O. Dorovskaya1,

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Presentation on theme: "MICROWAVE AND FIR SPECTROSCOPY OF DIMETHYLSULFIDE IN THE GROUND, FIRST AND SECOND EXCITED TORSIONAL STATES V. Ilyushin1, I. Armieieva1, O. Dorovskaya1,"— Presentation transcript:

1 MICROWAVE AND FIR SPECTROSCOPY OF DIMETHYLSULFIDE IN THE GROUND, FIRST AND SECOND EXCITED TORSIONAL STATES V. Ilyushin1, I. Armieieva1, O. Dorovskaya1, M. Pogrebnyak1, I. Krapivin1, E. Alekseev1 , R. Motiyenko2, L. Margulès2, F. Kwabia Tchana3, A. Jabri4, L. Manceron5, S. Bauerecker6, C. Maul6 1 Institute of Radio Astronomy of NASU, Kharkov, Ukraine 2 Laboratoire PhLAM, Université de Lille 1, France 3 LISA, Université Paris-Est Créteil, Université Paris Diderot, France 4Sorbonne Universités, MONARIS, Paris, France 5 Synchrotron SOLEIL, Ligne AILES, Gif-sur-Yvette, France 6 Institut für Physikalische und Theoretische Chemie, Technische Universität Braunschweig, Braunschweig, Germany

2 PAM_C2v_2tops computer program
Motivation =0.062 PAM_C2v_2tops computer program H = (1/4) knpqr1r2s1s2t1t2 Bknpqr1r2s1s2t1t2  {J2kJznJxpJyq[pAr1pBr2cos(3s1A) cos(3s2B)sin(3t1A)sin(3t2B) (-1)(n+q) pBr1pAr2cos(3s1B) cos(3s2A)sin(3t1B)sin(3t2A)] [(-1)(n+q)sin(3t2A)sin(3t1B)cos(3s2A)cos(3s1B)pAr2pBr sin(3t2B)sin(3t1A)cos(3s2B)cos(3s1A)pBr2pAr1]JyqJxpJznJ2k} =0.102

3 Motivation AA species only

4 MW spectrometer in Kharkiv
BWO, 34 – 150 GHz PLL IF = 25 MHz FM modulated synthesizer 25 MHz Klystron 3.4 – 5.2 GHz IF = 5 MHz Absorbing cell Amplifier Lock-in detector Sine wave synthesizer 7 – 120 KHz DAC DDS AD9851 30 – 60 MHz Band-pass amplifier MHz Synthesizer 360 MHz Frequency divider f/2 Frequency Doubler (optional) Detector Schottky Reference synthesizer MHz

5 The Lille THz spectrometer
Based on solid state sources Frequency multiplication technique Absorption cell – stainless steel tube 2.2 m Main detector InSb bolometer In the range 75 – 330 GHz solid state Schottky diode detectors Frequency multiplication chain in frequency range 150 – 990 GHz : Synthesizer Agilent E8257D GHz Active multiplier (VDI) x6 75–110GHz Multipl. Passifs (VDI) x2: 150 – 220 GHz x3: 225 – 330 GHz x5: 400 – 500 GHz x6: 500 – 660 GHz x9: 750 – 990 GHz Variable attenuator THz spectrometer

6 SOLEIL synchrotron

7 Fragment of submillimeter wave spectrum of dimethylsulfide
theory experiment theory experiment

8 Overview of the 15 = 1  0 torsional band of DMS
theory experiment 149.0 177.5 206.0 cm-1 163.25 191.75 220.25

9 Q-branch theory experiment 182.43 182.93 183.43 cm-1 182.68 183.18
183.68

10 Fragment of R-branch theory experiment 198.66 198.78 198.90 cm-1
198.72 198.84 198.96

11 Fragment of P-branch theory experiment 163.05 163.19 163.33 cm-1
163.12 163.26 163.40

12 Reassignment of the FIR spectra
AA transitions only A. Jabri, V. Van, H. V. L. Nguyen, H. Mouhib, F. Kwabia Tchana, L. Manceron, W. Stahl, and I. Kleiner, A&A 589, A127 (2016)

13 Overview of the data set fit quality
# lines in the fit, wrms = 0.88, Jmax=60, Kamax=30 Npar = 89 Current work A. Jabri et al., A&A 589, A127 (2016) Unc. # rms 5 kHz 98 4.7 kHz 99 5.5 kHz 10 kHz 3814 8.7 kHz 30 kHz 7871 24.1 kHz 40 kHz 300 27.3 kHz 305 52.7 kHz 50 kHz 7134 54.7 kHz 18 48.6/ 69.7 kHz 100 kHz 3547 68.0 kHz 180 84.6 kHz 200 kHz 29 90.0 kHz cm-1 1013 cm-1 578 cm-1 gs transitions rms=48.79 kHz 11= transitions rms=41.30 kHz 15 = transitions rms=48.80 kHz 15   transitions rms=39.22 kHz

14 SUMMARY OF THE FIT More than new lines were added to the dataset in the frequency range from 49 GHz to 660 GHz The dataset consists of microwave and 1013 FIR lines covering (15, 11) = (0,0),(0,1),(1,0) torsional states. The range of rotational quantum numbers is expanded up to J = 60 and Ka=30 Obtained theoretical model containing 89 parameters provides a fit within experimental error (weighted rms 0.88)

15 Comparison with ab initio calculations
Senent M. L., Puzzarini C., Dominguez-Gomez R., Carvajal M., Hochlaf M., 2014, J. Chem. Phys., 140, CCSD(T)/AVTZ level A. Jabri, V. Van, H. V. L. Nguyen, H. Mouhib, F. Kwabia Tchana, L. Manceron, W. Stahl, and I. Kleiner, A&A 589, A127 (2016) 15 = cm-1 CCSD/VTZ anharmonic 182 cm-1 11 = cm-1 CCSD/VTZ anharmonic 177 cm-1

16 Thank you for your attention
This work was done under support of the Volkswagen foundation. The assistance of Science and Technology Center in Ukraine is acknowledged (STCU partner project #P686).


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