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January 18, 2007

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Charles Chackerian, Jr.

Selection from peer-reviewed publications:

50. A. Levy, N. Lacome and C. Chackerian, Jr., "Chapter V, Collisional Line Mixing" in Spectroscopy of the Earth's Atmosphere and Interstellar Molecules (K. Narahari Rao and A. Weber, Eds.) Academic Press Inc. pp 261-337 (1992).

51. M. N. Spencer, C. Chackerian, Jr., C. Flannery, and J. I. Steinfeld, "Temperature Dependence of Nitrogen Broadening of Ozone n3 Rovibrational Transitions", Spectrochimica ACTA 48A, 1273-1281 (1992).

53. C. Chackerian, Jr., D. Goorvitch, A. Benidar, R. Farrenq, G. Guelachvili, P. M. Martin, M. C. Abrams and S. P. Davis, "Rovibrational Intensities and Electric Dipole Moment Function of the X 2P Hydroxyl Radical", J Quant. Spectrosc.Radiat. Transfer 48, 667-673 (1992).

54. D. Goorvitch, A. Goldman, R. H. Tipping, C. Chackerian, Jr., "The Hydroxyl Pure Rotational Transitions". J. Geophys. Res. 97, 20,771-20,786 (1992).

59. M. N. Spencer, C. Chackerian, Jr., C. Flannery, and J. I. Steinfeld, "Temperature Dependence of Oxygen Broadening of Ozone n3 Rovibrational Transitions", J. Quant. Spectrosc.Radiat. Transfer 49, 525-533 (1993).

62. D. Goorvitch and C. Chackerian, Jr., "Calculation of 12C16O and 13C16O X 1S+ Rovibrational Intensities for v ≤ 20 and J ≤150", Ap. J. Supplement 91, 483-489 (1994).

63. M. N. Spencer, C. Chackerian, Jr., L. P. Giver and L. R. Brown, "The Nitric Oxide Fundamental Band: Rovibrational Line Frequency and Shape Parameters," J. Mol. Spectrosc. 165, 506-524(1994).

67. T. A. Blake, C. Chackerian, Jr. and J. R. Podolske, "Prognosis For A Mid-Infrared Magnetic Rotation Spectrometer For The in situ Detection of Atmospheric Free Radicals," Applied Optics 35, 973-985 (1996).

68. L. P. Giver, C. Chackerian, Jr., M. N. Spencer, L. R. Brown and R. B. Wattson, "The Rovibrational Intensities of the (4001)¬(0000) Pentad Absorption Bands of 12C16O2 between 7284 and 7921 cm-1, J. Mol. Spectrosc. 175, 104-111 (1996).

69. M. N. Spencer, C. Chackerian, Jr., L. P. Giver and L. R. Brown. "Temperature Dependence of Nitrogen Broadening of the NO Fundamental Vibrational Band", J. Mol. Spectrosc. 181, 307-(1997).

72. C. Mahon and C. Chackerian, Jr. " Zeeman Tuning Rates for Q-Branch Transitions in the n3 Band of NO2", J. Mol. Spectrosc. 189, 276-282 (1998).

74. C. Chackerian, Jr., L. R. Brown, N. Lacome, and G. Tarrago, "Methyl Chloride n5 Region Line Shape Parameters and Rotational Constants for the n2, n5 and 2n3 Vibrational Bands", J. Mol. Spectrosc. 191, 148-157 (1998).

75. C. Chackerian, Jr., R. S. Freedman, L. P. Giver and L. R. Brown, "The NO Vibrational Fundamental Band O2-Broadening Coefficients" J. Mol. Spectrosc. 192, 215 (1998).

76. R. J. Kshirsagar, L. P. Giver, C. Chackerian. Jr., and L. R. Brown, "The Rovibrational Intensities of the 2n3 Band of 12C16O18O at 4639 cm-1, J. Quant. Spectrosc. Radiat. Transfer 61, 695-701 (1999).

80. R. J. Kshirsagar, L. P. Giver, and C. Chackerian. Jr., "Rovibrational Intensities of the (0003)-(1000) Dyad Absorption Bands of 12C16O2", J. Mol. Spectrosc. 199, 230-235 (2000).

81. L. P. Giver, C. Chackerian, Jr., and P. Varanasi, "Visible and near-infrared H216O line intensity corrections for HITRAN-96", J. Quant. Spectrosc. Radiat. 66, 101-105 (2000).