J/A+A/687/A69ivo://CDS.VizieR/J/A+A/687/A69doi:10.26093/cds/vizier.36870069CDSJozwiak H.Stolarczyk N.Stankiewicz K.Zaborowski M.Lisak D.,Wojtewicz Sz.Jankowski P.Patkowski K.Szalewicz K.Thibault F.,Gordon I.E.Wcislo P.2025-07-11T20:01:04Z2024-07-02T08:12:53ZCDS support team

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

cds-question@unistra.fratomic-physicsspectroscopyThe hydrogen deuteride (HD) molecule is an important deuterium tracer in astrophysical studies. The atmospheres of gas giants are dominated by molecular hydrogen, and the simultaneous observation of H2 and HD lines provides reliable information on the D/H ratios on these planets. The reference spectroscopic parameters play a crucial role in such studies. Under the thermodynamic conditions encountered in these atmospheres, spectroscopic studies of HD require not only the knowledge of line intensities and positions but also accurate reference data on pressure-induced line shapes and shifts. Our aim is to provide accurate collision-induced line-shape parameters for HD lines that cover any thermodynamic conditions relevant to the atmospheres of giant planets, namely any relevant temperature, pressure, and perturbing gas composition (the H_2_-He mixture). We performed quantum-scattering calculations on our new, highly accurate ab initio potential energy surface (PES), and we used scattering S matrices obtained in this way to determine the collision-induced line-shape parameters. We used cavity ring-down spectroscopy to validate our theoretical methodology. We report accurate collision-induced line-shape parameters for the pure rotational R(0), R(1), and R(2) lines, the most relevant HD lines for investigations of the atmospheres of the giant planets. Besides the basic Voigt-profile collisional parameters (i.e., the broadening and shift parameters), we also report their speed dependences and the complex Dicke parameter, which can influence the effective width and height of the HD lines up to almost a factor of 2 for giant planet conditions. The sub-percent-level accuracy reached in this work is a considerable improvement over previously available data. All the reported parameters (and their temperature dependences) are consistent with the HITRAN database format, hence allowing for the use of the HITRAN Application Programming Interface (HAPI) for generating the beyond-Voigt spectra of HD.2024A&A...687A..69Jhttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/687/A69CatalogResearchIsServedByTAP VizieR generic servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/A+A/687/A69https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/A+A/687/A69http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/A+A/687/A69https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/A+A/687/A69https://vizier.iucaa.in/viz-bin/votable?-source=J/A+A/687/A69http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/A+A/687/A69GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/A+A/687/A69/table1aGSXS for R(0) 0-0 line in HD + H2(j=0)qTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table1bGSXS for R(0) 0-0 line in HD + H2(j=1)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table1cGSXS for R(0) 0-0 line in HD + H2(j=2)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table1dGSXS for R(0) 0-0 line in HD + H2(j=3)qTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table1eGSXS for R(0) 0-0 line in HD + H2(j=4)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table1fGSXS for R(0) 0-0 line in HD + H2(j=5)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table2GSXS for R(0) 0-0 line in HD + HerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviInitial vibrational level of the active moleculephys.atmol.initial;phys.mol.vibrationintjiInitial rotational level of the active moleculephys.atmol.initial;phys.mol.rotationintvfFinal vibrational level of the active moleculephys.atmol.final;phys.mol.vibrationintjfFinal rotational level of the active moleculephys.atmol.final;phys.mol.rotationintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table3aGSXS for R(1) 0-0 line in HD + H2(j=0)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table3bGSXS for R(1) 0-0 line in HD + H2(j=1)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table3cGSXS for R(1) 0-0 line in HD + H2(j=2)viBottom vibrational level of the active moleculephysintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table3dGSXS for R(1) 0-0 line in HD + H2(j=3)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table3eGSXS for R(1) 0-0 line in HD + H2(j=4)qTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table3fGSXS for R(1) 0-0 line in HD + H2(j=5)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table4GSXS for R(1) 0-0 line in HD + HerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviInitial vibrational level of the active moleculephys.atmol.initial;phys.mol.vibrationintjiInitial rotational level of the active moleculephys.atmol.initial;phys.mol.rotationintvfFinal vibrational level of the active moleculephys.atmol.final;phys.mol.vibrationintjfFinal rotational level of the active moleculephys.atmol.final;phys.mol.rotationintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table5aGSXS for R(2) 0-0 line in HD + H2(j=0)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table5bGSXS for R(2) 0-0 line in HD + H2(j=1)jfTop rotational level of the active moleculephysintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table5cGSXS for R(2) 0-0 line in HD + H2(j=2)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table5dGSXS for R(2) 0-0 line in HD + H2(j=3)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table5eGSXS for R(2) 0-0 line in HD + H2(j=4)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table5fGSXS for R(2) 0-0 line in HD + H2(j=5)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table6GSXS for R(2) 0-0 line in HD + HerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviInitial vibrational level of the active moleculephys.atmol.initial;phys.mol.vibrationintjiInitial rotational level of the active moleculephys.atmol.initial;phys.mol.rotationintvfFinal vibrational level of the active moleculephys.atmol.final;phys.mol.vibrationintjfFinal rotational level of the active moleculephys.atmol.final;phys.mol.rotationintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table7Parameters for R(0) 0-0 line in HD + H2recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTTemperatureKphys.temperaturedoublegamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloatJ/A+A/687/A69/table8Parameters for R(0) 0-0 line in HD + HeTTemperatureKphys.temperaturedoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintgamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloatJ/A+A/687/A69/table9Parameters for R(1) 0-0 line in HD + H2recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTTemperatureKphys.temperaturedoublegamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloatJ/A+A/687/A69/table10Parameters for R(1) 0-0 line in HD + HerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTTemperatureKphys.temperaturedoublegamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloatJ/A+A/687/A69/table11Parameters for R(2) 0-0 line in HD + H2recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTTemperatureKphys.temperaturedoublegamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloatJ/A+A/687/A69/table12Parameters for R(2) 0-0 line in HD + HerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTTemperatureKphys.temperaturedoublegamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloatJ/A+A/687/A69/table13aGSXS for S(2) 2-0 line in D2 + H2(j=0)j2Initial rotational level of the perturber (H2)phys.atmol.levelintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table13bGSXS for S(2) 2-0 line in D2 + H2(j=1)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table13cGSXS for S(2) 2-0 line in D2 + H2(j=2)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table13dGSXS for S(2) 2-0 line in D2 + H2(j=3)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table13eGSXS for S(2) 2-0 line in D2 + H2(j=4)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table13fGSXS for S(2) 2-0 line in D2 + H2(j=5)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintqTensorial rank of the transition (R:q=1, S:q=2)phys.energy;phys.atmol.levelintviBottom vibrational level of the active moleculephysintjiBottom rotational level of the active moleculephysintvfTop vibrational level of the active moleculephysintjfTop rotational level of the active moleculephysintv2Initial vibrational level of the perturber (H2)phys.atmol.levelintj2Initial rotational level of the perturber (H2)phys.atmol.levelintEkinRelative kinetic energycm**-1phys.energy;phys.atmol.leveldoubleInelContribution to PBXS from inelastic events (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePBXSPressure broadening cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoublePSXSPressure shift cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleRDXSReal part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleIDXSImaginary part of the Dicke cross-section (in {AA}^2^ unit)0.01nm**2phys.atmoldoubleJ/A+A/687/A69/table14Parameters for S(2) 2-0 line in D2 + H2recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTTemperatureKphys.temperaturedoublegamma-0Pressure broadening coefficient0.001cm**-1.atm**-1phys.atmolfloatdelta-0Pressure shift coefficient0.001cm**-1.atm**-1phys.atmolfloatgamma-2Quadratic speed dependence of broadenning0.001cm**-1.atm**-1phys.atmolfloatdelta_2Quadratic speed dependence of shift0.001cm**-1.atm**-1phys.atmolfloatRe(nu-opt)Dicke parameter (real part)0.001cm**-1.atm**-1phys.atmoldoubleIm(nu-opt)Dicke parameter (imaginary part)0.001cm**-1.atm**-1phys.atmolfloat