J/ApJS/95/535ivo://CDS.VizieR/J/ApJS/95/535doi:10.26093/cds/vizier.20950535CDSGoorvitch D.1997-12-09T20:25:46Z1997-12-09T21:23:51ZCDS support team

CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France

cds-question@unistra.fratomic-physicsradio-astronomyA complete line list with improved accuracy for all the rotation- vibration transitions of the fundamental, first, and second overtone bands up to nu=20 and J=149 of the ground state X ^1^{Sigma}^+^ of the seven CO isotopes - 12C16O, 13C16O, 12C17O, 12C18O, 13C18O, 14C16O, and 13C17O - is made available to the astronomical community. A line list of the pure rotational transitions up to nu=5 and J=60 is also made available for these seven isotopes. This line list contains the transition frequency, the lower state energy, the Einstein A-value, the gf-value, the transition strength at 3000K or 1000K for the pure rotational transitions, the expectation value of the effective dipole moment operator, and the quantum numbers of each transition. Individual partition functions are reported in the temperature range of 500 to 10,000K. Author's Address: Goorvitch D. <goorvitch@cma.arc.nasa.gov> Space Sciences Division, NASA Ames Research Center, Moffett Field, CA 94035-10001994ApJS...95..535Ghttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJS/95/535CatalogResearchIsServedByTAP VizieR generic servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/ApJS/95/535https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJS/95/535http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJS/95/535https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJS/95/535https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJS/95/535http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJS/95/535GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapRadiodefaultJ/ApJS/95/535/table6Transition frequencies, gf values, and J values for the bandheads of the R-branch overtone bands of 12C16OrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintvLower state vibrational quantum numberphys.atmol.qnintsigma1Frequency, fundamentalcm**-1em.freqdoublelog(gf1)gf-value, fundamentalphys.atmol.wOscStrengthdoubleJ1J-value, fundamentalphys.atmol.qnintsigma2Frequency, first overtonecm**-1em.freqdoublelog(gf2)gf-value, first overtonephys.atmol.wOscStrengthdoubleJ2J-value, first overtonephys.atmol.qnintsigma3Frequency, second overtonecm**-1em.freqdoublelog(gf3)gf-value, second overtonephys.atmol.wOscStrengthdoubleJ3J-value, second overtonephys.atmol.qnintJ/ApJS/95/535/table7Rotationless dipole moments, M(0), for the pure rotational transitions (D)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintvVibrational quantum numberphys.atmol.qnintM26Rotationless dipole moment, 12C16ODphys.mol.dipoledoubleM36Rotationless dipole moment, 13C16ODphys.mol.dipoledoubleM28Rotationless dipole moment, 12C18ODphys.mol.dipoledoubleM27Rotationless dipole moment, 12C17ODphys.mol.dipoledoubleM38Rotationless dipole moment, 13C18ODphys.mol.dipoledoubleM46Rotationless dipole moment, 14C16ODphys.mol.dipoledoubleM37Rotationless dipole moment, 13C17ODphys.mol.dipoledoubleJ/ApJS/95/535/table8Polynomial fits to [F(m)]^{1/2} for the pure rotational transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintIsotopeCode for the isotope, e.g. '26' for 12C16Ometa.codecharvVibrational quantum numberphys.atmol.qnintb0b_0 coefficientstat.fit.paramdoubleb1b_1 coefficientstat.fit.paramdoubleb2b_2 coefficientstat.fit.paramdoubleb3b_3 coefficientstat.fit.paramdoubleb4b_4 coefficientstat.fit.paramdoubleJ/ApJS/95/535/table9Line list of 12C16O Delta v = +1 transitionslog(gf)gf-valuephys.atmol.wOscStrengthdoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintJ/ApJS/95/535/table10Line list of 12C16O Delta v = +2 transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoublelog(gf)gf-valuephys.atmol.wOscStrengthdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintJ/ApJS/95/535/table11Line list of 12C16O Delta v = +3 transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoublelog(gf)gf-valuephys.atmol.wOscStrengthdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintJ/ApJS/95/535/table12Complete line list of the pure rotational transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoublelog(gf)gf-valuephys.atmol.wOscStrengthdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintIsotopeCode for the isotope, e.g. '26' for 12C16Ometa.codecharJ/ApJS/95/535/table13Complete line list of the fundamental transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoublelog(gf)gf-valuephys.atmol.wOscStrengthdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintIsotopeCode for the isotope, e.g. '26' for 12C16Ometa.codecharJ/ApJS/95/535/table14Complete line list of the first overtone transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoublelog(gf)gf-valuephys.atmol.wOscStrengthdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintIsotopeCode for the isotope, e.g. '26' for 12C16Ometa.codecharJ/ApJS/95/535/table15Complete line list of the second overtone transitionslog(gf)gf-valuephys.atmol.wOscStrengthdoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaTransition frequencycm**-1phys.energy;phys.atmol.transitiondoubleR2Expectation value, effective electric dipole matrix operator squaredD**2phys.mol.dipoledoubleAEinstein transition probability (A-value)Hzphys.atmol.transProbdoubleELower state term energy, lowest level = 0cm**-1phys.energy;phys.mol.vibrationdoubleSStrength evaluated at T = 3000 Kcm/molspect.line.intensitydoublevuUpper state vibrational quantum numberphys.atmol.qnintvlLower state vibrational quantum numberphys.atmol.qnintType[RP] Transition typemeta.notecharJlLower state angular momentum numberphys.atmol.qnintIsotopeCode for the isotope, e.g. '26' for 12C16Ometa.codechar