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  Rotational transition frequencies of HCOOCH3 (Kobayashi+, 2013)
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1.J/ApJS/205/9/table1Pure rotational transition frequencies of cis-methyl formate in vt=2 analyzed by using the pseudo-principal-axis-method-(PAM) Hamiltonian model (Ohashi et al. 2004JMoSp.227...28O) (1953 rows)
2.J/ApJS/205/9/table3Pure rotational A-sublevel transition frequencies of cis-methyl formate in vt=2 analyzed by using Watson's A-reduced Hamiltonian (Equation (5)) (1012 rows)

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Column  Constraint Explain   (UCD)
  (ALL)recno  Record number assigned by the VizieR team. Should Not be used for identification. (meta.record)
  (1)S (char) [AE] Symmetry: the A or E torsional substates (phys.atmol)
   (ALL)J'   [2/40] The upper J quantum number (instr.det.qe;stat.max)
   (ALL)Ka'   [0/15] The upper Ka quantum number (phys.atmol.qn;stat.max)
   (ALL)Kc'   [0/37] The upper Kc quantum number (phys.atmol.qn;stat.max)
   (ALL)J"   [1/39] The lower J quantum number (instr.det.qe;stat.min)
   (ALL)Ka"   [0/15] The lower Ka quantum number (phys.atmol.qn;stat.min)
   (ALL)Kc"   [0/34] The lower Kc quantum number (phys.atmol.qn;stat.min)
   (ALL)Freq MHz [-168772.5/378357.1] The experimental frequency of the transition (em.freq;phys.atmol.transition)
  (1)f_Freq (char) [*] The * shows the transitions not included (meta.code)
   (ALL)O-C MHz [-0.23/0.44] The observed minus calculated value (

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 (i)indexed column
   (ALL)El cm-1 [0.4105/347.948] The lower state energy (Note G1)   (;phys.atmol.level)
   (ALL)Smu2 D+2 [0.07/89.51] The line strength (see equation (6)) (spect.line.intensity)
   (ALL)Ref (char) The source of measurement (Note G2)   (meta.bib)
  (2)all (char) Frequencies for this transition from the different methods (meta.ref.url)

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