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References for the molecule O₂

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. RouillÃ©, 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 XΣ 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 XΣ 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 XΣ 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 (X³Σ_g⁻, v = 0) state //J Mol Spectrosc 148, 447-452 (1991)
7.: Molecular Hamiltonian constants for the v″= 0 and v′= 0 of the XΣ state are from M. Mizushima, S. Yamamoto, Microwave absorption lines of ¹⁶O¹⁸O in its (X³Σ_g⁻, 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 a¹Δ_g 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 a¹Δ_g 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 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 aΔ state, the constants of K.W. Hillig II, C.C.W. Chiu, W.G. Read, E.A. Cohen, The pure rotation spectrum of a¹Δ_g 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 a¹Δ_g 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 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 aΔ_g 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 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 aΔg state, the constants of K.W. Hillig II, C.C.W. Chiu, W.G. Read, E.A. Cohen, The pure rotation spectrum of a¹Δ_g 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 a¹Δ_g 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 XΣ are from M. Mizushima, S. Yamamoto, Microwave absorption lines of ¹⁶O¹⁸O in its (X³Σ_g⁻, v = 0) state // J Mol Spectrosc 148, 447-452 (1991).
For the v′= 0 of the aΔ_g 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 (X³Σ_g⁻) from laser magnetic resonance spectra //J Mol Spectrosc 107 395-404 (1984)
17.: Molecular Hamiltonian constants for the v″=0 state of XΣ are from M. Mizushima, L.R. Zink, K.M. Evenson, Rotational structure of ¹⁶O₂, ¹⁶O¹⁷O, and ¹⁶O¹⁸O (X³Σ_g⁻) from laser magnetic resonance spectra // J Mol Spectrosc 107 395-404 (1984).
For the v′= 0 of the aΔ_g 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 XΣ_g⁻ 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)