Rotational levels of the (0 0 0) and (0 1 0) states of D216O from hot emission spectra in the 320–860 cm−1 region
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Herbert Over | Sergey A. Tashkun | Semen N. Mikhailenko | Vl.G. Tyuterev | S. Mikhailenko | V. Tyuterev | H. Over | E. Starikova | G. Mellau | G. Mellau | E. N Starikova | S. Tashkun
[1] C. Beard,et al. Two D2O Microwave Absorption Lines , 1952 .
[2] O. Polyansky. One-dimensional approximation of the effective rotational Hamiltonian of the ground state of the water molecule , 1985 .
[3] Camy-Peyret,et al. High-Lying Rotational Levels of Water: Comparison of Calculated and Experimental Energy Levels for (000) and (010) up to J = 25 and 21. , 1999, Journal of molecular spectroscopy.
[4] Manfred Winnewisser,et al. High-Temperature Infrared Measurements in the Region of the Bending Fundamental of H12C14N, H12C15N, and H13C14N , 2000 .
[5] Hu,et al. High-Resolution Fourier Transform Spectrum of the D(2)O Molecule in the Region of the Second Triad of Interacting Vibrational States. , 2000, Journal of molecular spectroscopy.
[6] J. Flaud,et al. The 2ν2, ν1 and ν3 bands of D216O. The ground state (000) and the triad of interacting states {(020), (100), (001)} , 1981 .
[7] M. Birk,et al. The rotational-torsional spectrum of carbodiimide: A probe for the unusual dynamics , 1989 .
[8] S. Mikhailenko,et al. Calculation of High Rotation Energies of the Water Molecule Using the Generating Function Model , 1995 .
[9] J. W. C. Johns,et al. High-resolution far-infrared (20–350-cm −1 ) spectra of several isotopic species of H 2 O , 1985 .
[10] O. Naumenko,et al. The 3ν2 Band of D216O , 2000 .
[11] Frank C. De Lucia,et al. Submillimeter spectroscopy of the major isotopes of water , 1984 .
[12] R. Toth. D216O and D218O Transition Frequencies and Strengths in the ν2 Bands , 1993 .
[13] Ji‐Xin Cheng,et al. High-Resolution Fourier-Transform Intracavity Laser Absorption Spectroscopy of D2O in the Region of the 4ν1+ν3 Band , 2002 .
[14] J. Flaud,et al. Atlas of the High‐Temperature Water Vapor Spectrum in the 3000 to 4000 cm−1 Region , 1983 .
[15] Winnewisser,et al. Climbing the Bending Vibrational Ladder in D13C15N by Hot Gas Emission Spectroscopy. , 1999, Journal of molecular spectroscopy.
[16] J. Bellet,et al. Application of Watson's centrifugal distortion theory to water and light asymmetric tops. General methods. Analysis of the ground state and the ν2 state of D2O16 , 1973 .
[17] S. Mikhailenko,et al. (0 0 0) and (0 1 0) States of H 2 18 O: analysis of rotational transitions in hot emission spectrum in the 400-850 cm -1 region , 2003 .
[18] P. Bernath,et al. Water on the sun. , 1995, Science.
[19] P. Bernath,et al. Hot Bands of Water in the ν2Manifold up to 5ν2-4ν2 , 1997 .
[20] J. Cox,et al. Millimeter‐Wave Lines of Heavy Water , 1956 .
[21] Rong-Long Wang,et al. Frequency Measurement of Pure Rotational Transitions of D(2)O from 0.5 to 5 THz. , 2001, Journal of molecular spectroscopy.
[22] Laurence S. Rothman,et al. HIGH-TEMPERATURE SPECTRUM OF H2O IN THE 720–1400cm-1 REGION , 1998 .
[23] S. Mikhailenko,et al. The 2ν2Band of Water: Analysis of New FTS Measurements and High-KaTransitions and Energy Levels☆ , 1997 .
[24] R. Strauch,et al. Water vapor spectrum near 600 GHz , 1970 .
[25] J. T. Massey,et al. SOME HEAVY WATER ROTATIONAL ABSORPTION LINES , 1953 .
[26] J. Flaud,et al. Line positions and intensities in theν2 band of D2O improvied pumped D2O laser frequencies , 1985 .
[27] Jingjing Zheng,et al. High-Resolution Fourier Transform Spectrum of D2O in the Region Near 0.97 μm , 2001 .
[28] V. Horneman,et al. High-resolution rotational absorption spectra of H 2 16 O, HD 16 O, and D 2 16 O between 110 and 500 cm -1 , 1995 .
[29] O. Naumenko,et al. Analysis of the D2O absorption spectrum near 2.5 μm , 1987 .
[30] E. Bekhtereva,et al. High-Resolution Study of the First Hexad of D2O , 2000 .
[31] S. Tashkun,et al. CDSD-1000, the high-temperature carbon dioxide spectroscopic databank , 2003 .
[32] E. Bekhtereva,et al. High-Resolution Study of the (v1 + 12v2 + v3 = 3) Polyad of Strongly Interacting Vibrational Bands of D2O , 2000 .
[33] V. I. Starikov,et al. Water Spectra in the Region 4200-6250 cm −1 , Extended Analysis of ν1 + ν2, ν2 + ν3, and 3ν2 Bands and Confirmation of Highly Excited States from Flame Spectra and from Atmospheric Long-Path Observations , 2002 .
[34] R. S. Williamson,et al. Experimental Energy Levels of the Water Molecule , 2001 .
[35] H. Sasada,et al. 1.5-μm DFB semiconductor laser spectroscopy of deuterated water , 1989 .
[36] J. Watson. Determination of Centrifugal Distortion Coefficients of Asymmetric‐Top Molecules , 1967 .
[37] Harry Partridge,et al. The determination of an accurate isotope dependent potential energy surface for water from extensive ab initio calculations and experimental data , 1997 .
[38] V. M. Devi,et al. Absolute line intensity measurements in the ν2 bands of HDO and D2O using a tunable diode laser spectrometer , 1986 .
[39] Harry Partridge,et al. Convergence testing of the analytic representation of an ab initio dipole moment function for water: Improved fitting yields improved intensities , 2000 .
[40] S. Clough,et al. Microwave Spectrum and Rotational Constants for the Ground State of D2O , 1970 .
[41] V. Tyuterev. The generating function approach to the formulation of the effective rotational Hamiltonian , 1992 .
[42] M. Winnewisser,et al. The Hot Band ν1 + 2ν2 + ν3 − ν2 of D216O , 1994 .
[43] M. Winnewisser,et al. The 3ν2 + ν3, ν1 + ν2 + ν3, ν1 + 3ν2, 2ν1 + ν2, and ν2 + 2ν3 Bands of D216O: The Second Hexade of Interacting States , 1993 .