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References for the molecule O2

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20.
W.S. Benedict, University of Maryland, private communication, 8/27/76.
21.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from G. Rouillé, G. Millot, R. Saint-Loup, H. Berger, High-resolution stimulated Raman spectroscopy of O2 // J Mol Spectrosc 154, 372-382 (1992).
For the v′= 0 of the bΣ state, the constants of D.L. Albritton, W.J. Harrop, A.L. Schmeltekopf, R.N. Zare, Resolution of the discrepancies concerning the optical and microwave values for B0 and D0 of the XΣg− state of O2 // J Mol Spectrosc 46, 103-118 (1973) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state.
22.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from G. Rouillé, G. Millot, R. Saint-Loup, H. Berger, High-resolution stimulated Raman spectroscopy of O2 // J Mol Spectrosc 154, 372-382 (1992).
For the v′= 1 of the bΣ state, the constants of D.L. Albritton, W.J. Harrop, A.L. Schmeltekopf, R.N. Zare, Resolution of the discrepancies concerning the optical and microwave values for B0 and D0 of the XΣg− state of O2 // J Mol Spectrosc 46, 103-118 (1973) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state.
23.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from G. Rouillé, G. Millot, R. Saint-Loup, H. Berger, High-resolution stimulated Raman spectroscopy of O2 // J Mol Spectrosc 154, 372-382 (1992).
For the v′= 2 of the bΣ state, the constants of D.L. Albritton, W.J. Harrop, A.L. Schmeltekopf, R.N. Zare, Resolution of the discrepancies concerning the optical and microwave values for B0 and D0 of the XΣg− state of O2 // J Mol Spectrosc 46, 103-118 (1973) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state.
24.
Molecular Hamiltonian constants for the v″= 1 state of XΣ are from G. Rouillé, G. Millot, R. Saint-Loup, H. Berger, High-resolution stimulated Raman spectroscopy of O2 // J Mol Spectrosc 154, 372-382 (1992).
For the v′= 1 of the bΣ state, the constants of D.L. Albritton, W.J. Harrop, A.L. Schmeltekopf, R.N. Zare, Resolution of the discrepancies concerning the optical and microwave values for B0 and D0 of the XΣg− state of O2 // J Mol Spectrosc 46, 103-118 (1973) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state.
25.
Molecular Hamiltonian constants for the v″= 1 state of XΣ are from G. Rouillé, G. Millot, R. Saint-Loup, H. Berger, High-resolution stimulated Raman spectroscopy of O2 // J Mol Spectrosc 154, 372-382 (1992).
For the v′= 0 of the bΣ state, the constants of D.L. Albritton, W.J. Harrop, A.L. Schmeltekopf, R.N. Zare, Resolution of the discrepancies concerning the optical and microwave values for B0 and D0 of the XΣg− state of O2 // J Mol Spectrosc 46, 103-118 (1973) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state.
26.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from M. Mizushima, S. Yamamoto, Microwave absorption lines of 16O18O in its (X3Σg−, v = 0) state // J Mol Spectrosc 148, 447-452 (1991).
For the v′= 0 of the bΣ state, the constants of H. Babcock, L. Herzberg, Fine structure of the red system of atmospheric oxygen bands // Astrophys J 108, 167-190 (1948) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state. Electronic term value is shifted by (-0.041-0.014) cm-1, unknown reference.
27.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from M. Mizushima, S. Yamamoto, Microwave absorption lines of 16O18O in its (X3Σg−, v = 0) state // J Mol Spectrosc 148, 447-452 (1991).
For the v′= 1 of the bΣ state, the constants of W.S. Benedict, University of Maryland, private communication, 8/27/76 are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state. Electronic term value is shifted by (-0.041-0.014) cm-1, unknown reference.
28.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from M. Mizushima, S. Yamamoto, Microwave absorption lines of 16O18O in its (X3Σg−, v = 0) state // J Mol Spectrosc 148, 447-452 (1991).
For the v′= 2 of the bΣ state, the constants from W.S. Benedict, University of Maryland (private communication) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state. Electronic term value is shifted by (-0.041-0.014) cm-1, unknown reference.
29.
Molecular Hamiltonian constants for the v″= 0 state of XΣ are from M. Mizushima, S. Yamamoto, Microwave absorption lines of 16O18O in its (X3Σg−, v = 0) state // J Mol Spectrosc 148, 447-452 (1991).
For the v′ = 1 of the bΣ state, the constants of H. Babcock, L. Herzberg, Fine structure of the red system of atmospheric oxygen bands // Astrophys J 108, 167-190 (1948) are used.
Vibrational and electronic term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Dunham zero point energy correction applied to zero point energy of upper vibrational state.
30.
R.L. Poynter, H.M. Pickett, Submillimeter, Millimeter, and Microwave Spectral Line Catalog  //JPL Publication 80-23, rev. 1 (1981)
31.
J.W. Brault, W.S. Benedict, Data from analysis of Kitt Peak observations, private communication (1978).
32.
K. Minschwaner, G.P. Anderson, L.A. Hall, K. Yoshino, Polynomial coefficients for calculating O2 Schumann-Runge cross sections at 0.5 cm−1 resolution //J Geophys Res D97, 10103-10108 (1992)
33.
K. Chance, K.W. Jucks, D.G. Johnson, W.A. Traub, The Smithsonian astrophysical observatory database SAO92 //JQSRT 52, 447-457 (1994)
34.
K. Yoshino, J.R. Esmond, Harvard-Smithsonian Center for Astrophysics, private communication (1994).
35.
L.R. Brown, C. Plymate, Experimental line parameters of the oxygen A band at 760 nm //J Mol Spectrosc 199, 166-179 (2000)
36.
C. Camy-Peyret, private communication based on
C. Camy-Peyret, S. Payan, P. Jeseck, Y. Té, T. Hawat, High resolution balloon-borne spectroscopy within the O2 A-band: observations and radiative transfer modeling // Proceedings of the International Radiation Symposium, St. Petersburg, July 24-29, 2000, Paper E4.
37.
M.-F. Mérienne, A. Jenouvrier, B. Coquart, M. Carleer, S. Fally, R. Colin, A.C. Vandaele, C. Hermans, Improved data set for the Herzberg band systems of 16O2 //J Mol Spectrosc 207, 120 (2001)
38.
Blended lines from M.-F. Mérienne, A. Jenouvrier, B. Coquart, M. Carleer, S. Fally, R. Colin, A.C. Vandaele, C. Hermans, Improved data set for the Herzberg band systems of 16O2 // J Mol Spectrosc 207, 120 (2001).
39.
D.J. Robichaud, J.T. Hodges, P. Masłowski, L.Y. Yeung, M. Okumura, C.E. Miller, L.R. Brown, High-accuracy transition frequencies for the O2 A-band //J Mol Spectrosc 251, 27-37 (2008)
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