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THE MILLIMETER-WAVE SPECTRUM OF VINYL ACETATE
Grupo de Espectroscopía Molecular, Lab. de Espectroscopia y Bioespectroscopia Edificio Quifima, Unidad Asociada CSIC, Universidad de Valladolid, Valladolid, Spain Departamento de Astrofísica, Centro de Astrobiología, CAB, CSIC-INTA, Madrid, Spain CNRS et Universités Paris Est et Paris Diderot, Laboratoire Interuniversitaire des Systèmes Atmosphériques (LISA), Creteil, France THE MILLIMETER-WAVE SPECTRUM OF VINYL ACETATE Lucie Kolesniková, Isabel Peña, José L. Alonso, José Cernicharo, Belén Tercero, Isabelle Kleiner International Symposium on Molecular Spectroscopy, June 16 20, 2014 Champaign-Urbana, Illinois, USA
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Introduction and motivation
Methyl acetate (CH3COOCH3) Gauche-ethyl formate (g-CH3CH2OCOH) detected in ORION KLa detected in Sgr B2b a Tercero B. , Kleiner I., Cernicharo J. , Nguyen H. V. L., Lopez A. , and Muñoz Caro G. M., 2013, ApJ. 770, L13. b Belloche, A., Garrod, R. T., Műller, H. S. P., et al. 2009, A&A, 499, 215.
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Introduction and motivation
Methyl acetate (CH3COOCH3) Gauche-ethyl formate (g-CH3CH2OCOH) Methyl acetate (CH3COOCH3) Gauche-ethyl formate (g-CH3CH2OCOH) Vinyl acetate (CH3COOCHCH2) – one of the simplest unsaturated carboxylic ester Previous data up to 77 GHzc → new data → search in Orion KL detected in ORION KLa detected in Sgr B2b acetate containing molecules are potential candidates a Tercero B. , Kleiner I., Cernicharo J. , Nguyen H. V. L., Lopez A. , and Muñoz Caro G. M., 2013, ApJ. 770, L13. b Belloche, A., Garrod, R. T., Műller, H. S. P., et al. 2009, A&A, 499, 215. c Velino B., Maris A., Melandri S., Caminati W. J Mol. Spectrosc. 256 (2009) 228 – 231.
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Vinyl acetate molecule
Predicted conformersb DE = 0 cm1 DE = 1060 cm1 DE = 2313 cm1 b Velino B., Maris A., Melandri S., Caminati W. J Mol. Spectrosc. 256 (2009) 228 – 231.
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Vinyl acetate molecule
MP2/ g(d,p): ma = 0.04 D mb = D mc = 0.09 D The most stable conformer Previous data (61 – 77 GHz)b predictions (BELGI-Cs) Velino et. al.b: V3 = (93) cm1 A-E splitting b Velino B., Maris A., Melandri S., Caminati W. J Mol. Spectrosc. 256 (2009) 228 – 231.
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CP-FTMW spectra: experiment
CP-FTMW spectrometer (6 – 18 GHz)c Supersonic Expansion 2 nozzels Ne carrier gas (2 bar) Broadband FT-MW spectrometer c S. Mata I. Peña, C. Cabezas, J. C. López and J. L. Alonso. J. Mol. Spectrosc. 280 (2012) 91–96
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CP-FTMW spectra: analysis
6 – 18 GHz
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CP-FTMW spectra: analysis
6 – 18 GHz 2 1 1 2 0 2 1 1 1 0 0 0 2 1 2 1 0 1 1 1 0 1 0 1 A E E A E A A E 3 1 2 3 0 3 A E
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CP-FTMW spectra: analysis
6 – 18 GHz 2 1 1 2 0 2 1 1 1 0 0 0 2 1 2 1 0 1 1 1 0 1 0 1 A E E A E A A E 3 1 2 3 0 3 A E
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CP-FTMW spectra: analysis
6 – 18 GHz 2 1 1 2 0 2 1 1 1 0 0 0 2 1 2 1 0 1 1 1 0 1 0 1 A E E A E A A E 3 1 2 3 0 3 A E Parent species A-lines: 1 0 1 13C3 13C2 13C1 13C4 18O1 18O2
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CP-FTMW spectra: analysis
6 – 18 GHz 2 1 1 2 0 2 1 1 1 0 0 0 2 1 2 1 0 1 1 1 0 1 0 1 A E E A E A A E 3 1 2 3 0 3 A E assignments of the transitions of the parent species and isotopologues search for the second conformer Parent species A-lines: 1 0 1 13C3 13C2 13C1 13C4 18O1 18O2
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CP-FTMW spectra: results
A-species rotational constants (MHz) Parent species 13C1 13C2 13C3 13C4 18O1 18O2 A (86) (92) (98) (12) (58) (11) (23) B (16) (46) (21) (17) (27) (91) (24) C (17) (27) (29) (69) (16) (48) (12) Atom Substitution coordinates (Å) (assumption of the symmetry plane) |a| |b| C1 (58) (57) C2 (11) (51) C3 (17) 0.080 (19) C4 (74) (16) O1 (57) (29) O2 (14) (12)
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MMW spectra: experiment
MMW and sub-MMW spectrometer (50 – 1000 GHz) 129 – 360 GHz room temperature 20 mbar
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MMW spectra: experiment
MMW and sub-MMW spectrometer (50 – 1000 GHz) 129 – 360 GHz room temperature 20 mbar Synthesizer Sample cells Lock-in amplifier AM chains Lens
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MMW spectra: experiment
MMW and sub-MMW spectrometer (50 – 1000 GHz) Roof-top mirror Detector Synthesizer Sample cells Lock-in amplifier AM chains Lens
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MMW spectra: analysis MMW spectrum E A E A E A E A E A A
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MMW spectra: analysis AABS package: ncent (MHz) Dn (MHz)
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MMW spectra: analysis E A E A E A E A Ka’’ = 3, 4 Ka’’ = 2, 3
ncent (MHz) E A E A E A E A Dn (MHz)
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MMW spectra: analysis J’’ = 95, Ka’’ = 16 J’’ = 95, Ka’’ = 10
ncent (MHz) E A E A E A E A CP-FTMW + MMW spectra > transitions (A-species) J’’ = 95, Ka’’ = 16 > 900 transitions (E-species) J’’ = 95, Ka’’ = 10 BELGI-Cs code (rho-axis method) Dn (MHz)
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CP-FTMW + MMW spectra: results
Operatora Constant Unit Value Pa2 A cm-1 (31) Pb2 B (11) Pc2 C (45) {Pa,Pb} Dab (45) {Pa,Pc}(sin3) Dac (13) -P4 DJ x 10-8 (48) -Pa4 DK x 10-6 (46) -2P2(Pb2-Pc2) J x 10-9 (24) -2Pa2(Pb2-Pc2) K x 10-8 0.957 (17) P2 F [ ] (1/2)(1-cos3) V3 (44) PaP unitless (35) P 2 (Pa Pb + Pb Pa) Dab x 10-5 0.638 (35) (1-cos3)Pa2 k5 x 10-2 (94) (1-cos3)P2 FV x 10-3 (75) (1-cos3)(Pb2-Pc2) c2 x 10-4 (79) (1-cos3){Pa,Pb} dAB (60) PgPa P2 Lv (44) P4Pa2 HJK x 10-13 0.270 (40) Current fit: J’’ = 75 18 floated torsion-rotation parameters F constant fixed to the value obtained by XIAM (Velino B., Maris A., Melandri S., Caminati W. J Mol. Spectrosc. 256 (2009) 228 – 231.) a In the rho-axis system
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CP-FTMW + MMW spectra: results
Operatora Constant Unit Value Pa2 A cm-1 (31) Pb2 B (11) Pc2 C (45) {Pa,Pb} Dab (45) {Pa,Pc}(sin3) Dac (13) -P4 DJ x 10-8 (48) -Pa4 DK x 10-6 (46) -2P2(Pb2-Pc2) J x 10-9 (24) -2Pa2(Pb2-Pc2) K x 10-8 0.957 (17) P2 F [ ] (1/2)(1-cos3) V3 (44) PaP unitless (35) P 2 (Pa Pb + Pb Pa) Dab x 10-5 0.638 (35) (1-cos3)Pa2 k5 x 10-2 (94) (1-cos3)P2 FV x 10-3 (75) (1-cos3)(Pb2-Pc2) c2 x 10-4 (79) (1-cos3){Pa,Pb} dAB (60) PgPa P2 Lv (44) P4Pa2 HJK x 10-13 0.270 (40) New laboratory data up to 360 GHz principal axis-system New set of the spectroscopic constants Current fit: J’’ = 75 18 floated torsion-rotation parameters F constant fixed to the value obtained by XIAM Search for the vinyl acetate in Orion KL (Velino B., Maris A., Melandri S., Caminati W. J Mol. Spectrosc. 256 (2009) 228 – 231.) a In the rho-axis system
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Molecular Astrophysics
Acknowledgements Grants CTQ , AYA and AYA Grant VA070A08 CSD Molecular Astrophysics …and all the members of the
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