Comparison between theoretical calculations and high-resolution measurements of pressure broadening for near-infrared water spectra
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Jonathan Tennyson | A. D. Bykov | Joseph T. Hodges | Nina N. Lavrentieva | L. N. Sinitsa | Daniel Lisak | R. Tolchenov | J. Hodges | J. Tennyson | R. Barber | L. Sinitsa | N. Lavrentieva | A. Bykov | D. Lisak | Robert J. Barber | Roman N. Tolchenov | Joseph T. Hodges | Daniel Lisak | A. Bykov | J. Tennyson | R. Barber
[1] T. Wilkerson,et al. Water absorption lines, 931-961 nm - Selected intensities, N2-collision-broadening coefficients, self-broadening coefficients, and pressure shifts in air , 1982 .
[2] J. Buldyreva,et al. Semiclassical calculations with exact trajectory for N2 rovibrational Raman linewidths at temperatures below 300 K , 1999 .
[3] Paul R. Berman,et al. Speed-dependent collisional width and shift parameters in spectral profiles , 1972 .
[4] Jonathan Tennyson,et al. The Water Vapor Spectrum in the Region 8600-15 000 cm(-1): Experimental and Theoretical Studies for a New Spectral Line Database. , 2001, Journal of molecular spectroscopy.
[5] J. Tennyson,et al. A PROGRAM SUITE FOR THE CALCULATION OF RO-VIBRATIONAL SPECTRA OF TRIATOMIC-MOLECULES , 1989 .
[6] Jonathan Tennyson,et al. Spectroscopically determined potential energy surface of H216O up to 25 000 cm−1 , 2003 .
[7] J. Tennyson,et al. Ab initio calculation of the rotation–vibration energy levels of H3+ and its isotopomers to spectroscopic accuracy , 1999 .
[8] J. Tennyson,et al. High-Accuracy ab Initio Rotation-Vibration Transitions for Water , 2003, Science.
[9] Temkin,et al. Effect of speed-changing collisions on spectral line shape. , 1993, Physical review. A, Atomic, molecular, and optical physics.
[10] Ann Carine Vandaele,et al. Water vapor line parameters in the 13 000-9250 cm-1 region. , 2003 .
[11] V. Saveliev,et al. Half-width temperature dependence of nitrogen broadened lines in the ν2 band of H2O , 2004 .
[12] J. Hodges,et al. Frequency-stabilized cavity ring-down spectrometer for high-sensitivity measurements of water vapor concentration , 2006 .
[13] J. Hodges,et al. Comparison of semiclassical line-shape models to rovibrational H2O spectra measured by frequency-stabilized cavity ring-down spectroscopy , 2006 .
[14] G. Wlodarczak,et al. Lineshape study of the J =3←2 rotational transition of CO perturbed by N 2 and O 2 , 2000 .
[15] B. Lemoine,et al. Infrared HCN Lineshapes as a Test of Galatry and Speed-Dependent Voigt Profiles , 2002 .
[16] Edward F. Valeev,et al. CVRQD ab initio ground-state adiabatic potential energy surfaces for the water molecule. , 2006, The Journal of chemical physics.
[17] J. Hodges,et al. Frequency-stabilized single-mode cavity ring-down apparatus for high-resolution absorption spectroscopy , 2004 .
[18] Joseph T. Hodges,et al. High-resolution cavity ring-down spectroscopy measurements of blended H2O transitions , 2007 .
[19] A. Pine. Line mixing sum rules for the analysis of multiplet spectra. , 1997 .
[20] T. Mexia,et al. Author ' s personal copy , 2009 .
[21] Yu. N. Ponomarev,et al. Pressure broadening and shift coefficients of H2O due to perturbation by N2, O2, H2 and He in the 1.39 μm region: experiment and calculations , 2004 .
[22] Antonio Sasso,et al. An accurate comparison of lineshape models on H2O lines in the spectral region around 3 μm , 2004 .
[23] L. Galatry,et al. Simultaneous Effect of Doppler and Foreign Gas Broadening on Spectral Lines , 1961 .
[24] Alain Valentin,et al. Diode-Laser Spectroscopy: Line Profiles of H2O in the Region of 1.39 μm , 2001 .
[25] A. Pine. Line shape asymmetries in Ar‐broadened HF(v=1–0) in the Dicke‐narrowing regime , 1994 .
[26] V. Malathy Devi,et al. Spectroscopic challenges for high accuracy retrievals of atmospheric CO2 and the Orbiting Carbon Observatory (OCO) experiment , 2005 .
[27] M. Nelkin,et al. Simple Binary Collision Model for Van Hove's G s ( r , t ) , 1964 .
[28] 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 .
[29] J. Tennyson,et al. A high-accuracy computed water line list , 2006, astro-ph/0601236.
[30] D. Schwenke. Variational Calculations of Rovibrational Energy Levels and Transition Intensities for Tetratomic Molecules , 1996 .
[31] Robert A. Toth,et al. Measurements and analysis (using empirical functions for widths) of air- and self-broadening parameters of H2O , 2005 .
[32] Andrew G. Glen,et al. APPL , 2001 .
[33] Sergei G. Rautian,et al. Reviews of Topical Problems: the Effect of Collisions on the Doppler Broadening of Spectral Lines , 1967 .
[34] G. Blanquet,et al. On the Speed-Dependent Hard Collision Lineshape Models: Application to C2H2 Perturbed by Xe , 1997, Journal of molecular spectroscopy.
[35] D. Robert,et al. Short range force effects in semiclassical molecular line broadening calculations , 1979 .
[36] R. Tolchenov,et al. A new ab initio ground-state dipole moment surface for the water molecule. , 2008, The Journal of chemical physics.
[37] S. Tashkun,et al. CDSD-1000, the high-temperature carbon dioxide spectroscopic databank , 2003 .
[38] A. S. Pine,et al. Asymmetries and correlations in speed-dependent Dicke-narrowed line shapes of argon-broadened HF , 1999 .
[39] May,et al. Line-shape analysis of speed-dependent collisional width inhomogeneities in CO broadened by Xe, N2, and He. , 1995, Physical review. A, Atomic, molecular, and optical physics.
[40] Jonathan Tennyson,et al. The Water Vapor Spectrum in the Region 8600-15 000 cm(-1): Experimental and Theoretical Studies for a New Spectral Line Database. , 2001, Journal of molecular spectroscopy.
[41] G. G. Stokes. "J." , 1890, The New Yale Book of Quotations.
[42] R. Ciuryło,et al. Response of scanning Fabry-Pèrot interferometer to the speed dependent Voigt profile , 1995 .
[43] J. Hodges,et al. Automated high-resolution frequency-stabilized cavity ring-down absorption spectrometer , 2005 .
[44] Robert A. Toth,et al. Measurements of positions, strengths and self-broadened widths of H2O from 2900 to 8000 cm−1: line strength analysis of the 2nd triad bands , 2005 .
[45] R. Blackmore. A modified Boltzmann kinetic equation for line shape functions , 1987 .
[46] G. Rusciano,et al. Speed-dependent and correlation effects on the line shape of acetylene (8 pages) , 2005 .
[47] J. Hodges,et al. High-Precision Pressure Shifting Measurement Technique Using Frequency-Stabilized Cavity Ring-Down Spectroscopy , 2008 .
[48] Robert A. Toth,et al. Empirical Line Parameters of H216O near 0.94 μm: Positions, Intensities and Air-Broadening Coefficients , 2002 .
[49] R. W. Nicholls,et al. Relative band strengths for the AlO blue-green system , 1969 .
[50] C. J. Tsao,et al. Line-widths of pressure-broadened spectral lines , 1962 .
[51] May,et al. Line Mixing and Broadening in the Raman Q Branch of HD at 304.6 K. , 1998, Journal of molecular spectroscopy.
[52] J. Drummond,et al. Spectral line shape of the P(2) transition in CO-Ar: Uncorrelated ab initio calculation , 2002 .
[53] Jonathan Tennyson,et al. DVR3D: a program suite for the calculation of rotation-vibration spectra of triatomic molecules , 2004, Comput. Phys. Commun..
[54] J. Hartmann,et al. Collisional parameters of H2O lines : Velocity effects on the line-shape , 2007 .
[55] R. Dicke. The effect of collisions upon the Doppler width of spectral lines , 1953 .
[56] 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 .
[57] S. Neshyba,et al. Fully complex implementation of the Robert–Bonamy formalism: Half widths and line shifts of H2O broadened by N2 , 1996 .
[58] Jonathan Tennyson,et al. Spectroscopically determined potential energy surfaces of the H216O, H217O, and H218O isotopologues of water , 2006 .