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References for the molecule O2

Publication topic
Displaying 1-20 of 48 results.
0.
L.S. Rothman, R.R. Gamache, A. Goldman, L.R. Brown, R.A. Toth, H.M. Pickett, R.L. Poynter, J.-M. Flaud, C. Camy-Peyret, A. Barbe, N. Husson, C.P. Rinsland, M.A.H. Smith, The HITRAN database: 1986 edition //Appl Opt 26, 4058-4097 (1987)
1.
G. Rouillé, G. Millot, R. Saint-Loup, H. Berger, High-resolution stimulated Raman spectroscopy of O2 //J Mol Spectrosc 154, 372-382 (1992)
2.
P.H. Krupenie, The spectrum of molecular oxygen //J Phys Chem Ref Data 1, 423-534 (1972)
3.
Molecular Hamiltonian constants for the v″= 0 and v′= 0 of the state 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).
4.
Molecular Hamiltonian constants for the v″= 0 and v′= 1 of the state 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).
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972), upper vibrational state energy shifted to agree with band center of G. Rouillé et al. for (1←0) band.
5.
Molecular Hamiltonian constants for the v″= 1 and v′= 1 of the state 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).
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972), upper vibrational state energy shifted to agree with band center of G. Rouillé et al. for (1←0) band.
6.
M. Mizushima, S. Yamamoto, Microwave absorption lines of 16O18O in its (X3Σg, v = 0) state //J Mol Spectrosc 148, 447-452 (1991)
7.
Molecular Hamiltonian constants for the v″= 0 and v′= 0 of the state are from M. Mizushima, S. Yamamoto, Microwave absorption lines of 16O18O in its (X3Σg, v = 0) state // J Mol Spectrosc 148, 447-452 (1991).
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972).
8.
K.W. Hillig II, C.C.W. Chiu, W.G. Read, E.A. Cohen, The pure rotation spectrum of a1Δg O2 //J Mol Spectrosc 109, 205-206 (1985)
9.
A. Scalabrin, R.J. Saykally, K.M. Evenson, H.E. Radford, M. Mizushima, Laser magnetic resonance measurement of rotational transitions in the metastable a1Δg state of oxygen //J Mol Spectrosc 89, 344-351 (1981)
10.
J.W. Brault, Kitt Peak National Solar Observatory, private communication (1982).
11.
Molecular Hamiltonian constants for the v″=0 state of 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 aΔ state, the constants of K.W. Hillig II, C.C.W. Chiu, W.G. Read, E.A. Cohen, The pure rotation spectrum of a1Δg O2 // J Mol Spectrosc 109, 205-206 (1985) are used in the formalism of A. Scalabrin, R.J. Saykally, K.M. Evenson, H.E. Radford, M. Mizushima, Laser magnetic resonance measurement of rotational transitions in the metastable a1Δg state of oxygen // J Mol Spectrosc 89, 344-351 (1981).
Vibrational term values are from  P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Upper vibrational state energy shifted by -0.002788 cm-1 to agree with data of J.W. Brault, Kitt Peak National Solar Observatory, private communication (1982).
12.
Molecular Hamiltonian constants for the v″= 0 state of 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 aΔg state the constants of J.W. Brault, Kitt Peak National Solar Observatory, private communication (1982) are used.
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Upper vibrational state energy shifted by -0.050385 cm-1 to agree with data of J.W. Brault, Kitt Peak National Solar Observatory, private communication (1982).
13.
Molecular Hamiltonian constants for the v′= 1 state of 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 aΔg state, the constants of K.W. Hillig II, C.C.W. Chiu, W.G. Read, E.A. Cohen, The pure rotation spectrum of a1Δg O2 // J Mol Spectrosc 109, 205-206 (1985) are used in the formalism of A. Scalabrin, R.J. Saykally, K.M. Evenson, H.E. Radford, M. Mizushima, Laser magnetic resonance measurement of rotational transitions in the metastable a1Δg state of oxygen // J Mol Spectrosc 89, 344-351 (1981).
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Upper vibrational state energy shifted by -0.002788 cm-1 to be consistent with the (0←0) transitions.
14.
L. Herzberg, G. Herzberg, Fine structure of the infrared atmospheric oxygen bands //Astrophys J 105, 353-359 (1947)
15.
Molecular Hamiltonian constants for the v″= 0 state of 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 aΔg state, the constants of L. Herzberg, G. Herzberg, Fine structure of the infrared atmospheric oxygen bands // Astrophys J 105, 353-359 (1947) are used.
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Upper vibrational state energy shifted by +0.29573 cm-1 to agree with data of J.W. Brault, Kitt Peak National Solar Observatory, private communication (1982).
16.
M. Mizushima, L.R. Zink, K.M. Evenson, Rotational structure of 16O2, 16O17O, and 16O18O (X3Σg) from laser magnetic resonance spectra //J Mol Spectrosc 107 395-404 (1984)
17.
Molecular Hamiltonian constants for the v″=0 state of are from M. Mizushima, L.R. Zink, K.M. Evenson, Rotational structure of 16O2, 16O17O, and 16O18O (X3Σg) from laser magnetic resonance spectra // J Mol Spectrosc 107 395-404 (1984).
For the v′= 0 of the aΔg state, the constants of L. Herzberg, G. Herzberg, Fine structure of the infrared atmospheric oxygen bands // Astrophys J 105, 353-359 (1947) are used.
Vibrational term values are from P.H. Krupenie, The spectrum of molecular oxygen // J Phys Chem Ref Data 1, 423-534 (1972). Upper vibrational state energy shifted by +0.15634 cm-1 to agree with data of J.W. Brault, Kitt Peak National Solar Observatory, private communication (1982).
18.
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)
19.
H. Babcock, L. Herzberg, Fine structure of the red system of atmospheric oxygen bands //Astrophys J 108, 167-190 (1948)