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J/ApJS/169/28 Rotational transitions of Methyl carbamate (Groner+, 2007)
The millimeter- and submillimeter-wave spectrum of methyl carbamate [CH3OC(:O)NH2]. Groner P., Winnewisser M., Medvedev I.R., De Lucia F.C., Herbst E., Sastry K.V.L.N. <Astrophys. J. Suppl. Ser., 169, 28-36 (2007)> =2007ApJS..169...28G
ADC_Keywords: Atomic physics ; Millimetric/submm sources ; Spectroscopy Keywords: catalogs - submillimeter - techniques: spectroscopic Abstract: The rotational-torsional spectrum of the syn conformer of methyl carbamate [CH3OC(:O)NH2], an isomer of the essential amino acid glycine [NH2CH2C(:O)OH], has been recorded at room temperature in the spectral region from 79 to 371GHz. Methyl carbamate possesses a methyl group internal rotor, which gives rise to A and E torsional substates, and associated splittings in the rotational spectrum. Almost 6000 new rotational transitions arising from the vibrational ground state have been assigned, about half of them belonging to the E torsional substate. The Fast Scan Submillimeter-wave Spectroscopic Technique (FASSST) spectrometer at the Ohio State University was used for the present measurements File Summary:
FileName Lrecl Records Explanations
ReadMe 80 . This file table2.dat 59 6365 Assigned and fitted rotational transition frequencies of methyl carbamate in its ground vibrational state table4.dat 51 13665 Predicted rotational-transition frequencies for methyl carbamate in its ground vibrational state
See also: J/A+A/406/L47 : 17OH spin-rotation transition frequencies (Polehampton+ 2003) J/ApJ/500/1059 : Dimethyl ether transitions frequencies (Groner+, 1998) J/ApJS/162/428 : n-propanol transition frequencies (Maeda+, 2006) J/ApJS/166/650 : mm/submm spectrum of iso-propanol (Maeda+, 2006) Byte-by-byte Description of file: table2.dat
Bytes Format Units Label Explanations
1 I1 --- sig1 [0/1] Symmetry number (0=A-state, 1=E-state) 3- 4 I2 --- J1 The J upper state 6- 7 I2 --- Ka1 The Ka upper state 9- 10 I2 --- Kc1 The Kc upper state 12- 13 I2 --- J2 The J lower state 15- 16 I2 --- Ka2 The Ka lower state 18- 19 I2 --- Kc2 The Kc lower state 21- 31 F11.4 MHz Freq Frequency of transition 33- 36 F4.2 --- Coeff ? Coefficient of linear combination in blended transitions 38- 40 F3.1 MHz e_Freq Estimated experimental uncertainty in Freq (1) 42- 49 F8.4 MHz (O-C) Residual in least-squares fit 51- 57 F7.4 MHz (O-C)B ? Residual of blend in least-squares fit 59 A1 --- r_Freq [BM] Source of experimental frequency if not from FASSST measurements (2)
Note (1): Frequency received zero weight in least-squares fit if e_Freq=0. Note (2): Experimental frequencies from sources B and M were available with two digits following the decimal place. Experimental frequencies between 79 and 118GHz were available with three digits following the decimal place. Com is defined as: B = Bakri et al. (2002, J. Mol. Spectrosc., 215, 312), M = Marstokk & Moellendal (1999, Acta Chem. Scandinavica, 53, 79).
Byte-by-byte Description of file: table4.dat
Bytes Format Units Label Explanations
1 I1 --- sig1 [0/1] Symmetry number (0=A-state, 1=E-state) 3- 4 I2 --- J1 The J upper state 6- 7 I2 --- Ka1 The Ka upper state 9- 10 I2 --- Kc1 The Kc upper state 12- 13 I2 --- J2 The J lower state 15- 16 I2 --- Ka2 The Ka lower state 18- 19 I2 --- Kc2 The Kc lower state 21- 30 F10.3 MHz Freq Frequency of transition 32- 36 F5.3 MHz e_Freq Estimated uncertainty in Freq 38- 43 F6.3 --- S Line strength (b-type) 45- 51 F7.3 cm-1 Eup/hc Upper state energy
History: From electronic version of the journal
(End) Greg Schwarz [AAS], Marianne Brouty [CDS] 15-Dec-2008
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