HITRAN on the Web

Guest |

References for the molecule NH₃

Displaying 1-15 of 15 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. Guelachvili, A.H. Abdullah, N. Tu, K. Narahari Rao, Å . Urban, D. PapouÅ¡ek, Analysis of high-resolution Fourier transform spectra of ¹⁴NH₃ at 3.0 μm //J Mol Spectrosc 133, 345-364 (1989)
2.: Å . Urban, N. Tu, K. Narahari Rao, G. Guelachvili, Analysis of high-resolution Fourier transform spectra of ¹⁴NH₃ at 2.3 μm //J Mol Spectrosc 133, 312-330 (1989)
3.: I. Kleiner, G. Tarrago, L.R. Brown, Positions and intensities in the 3ν₂/ν₂ + ν₄ vibrational system of ¹⁴NH₃ near 4 μm //J Mol Spectrosc 173, 120-145 (1995)
4.: L.R. Brown, J.S. Margolis, Empirical line parameters of NH₃ from 4791 to 5294 cm⁻¹ //JQSRT 56, 283-294 (1996)
5.: C. Cottaz, I. Kleiner,G. Tarrago, L.R. Brown, J.S. Margolis, P.L. Poynter, H.M. Pickett, T. Fouchet, P. Drossart, Line positions and intensities in the 2ν₂/ν₄ vibrational system of ¹⁴NH₃ near 5–7 μm //J Mol Spectrosc 203, 285-309 (2000)
6.: C. Cottaz, G. Tarrago, I. Kleiner, L.R. Brown, Assignments and intensities of ¹⁴NH₃ hot bands in the 5- to 8-μm (3ν₂−ν₂, ν₂+ν₄−ν₂) and 4-μm (4ν₂−ν₂, ν₁−ν₂, ν₃−ν₂ and 2ν₄−ν₂) regions //J Mol Spectrosc 209, 30-49 (2001)
7.: C. Cottaz, 4-μm hot bands (thesis, U. Paris-Sud).
8.: Rotational, ν₂- ν₂, and ν₂-ground state prediction via John Pearson, JPL (private communication, 2000).
9.: I. Kleiner, L.R. Brown, G. Tarrago, Q.-L. Kou, N. Picque, G. Guelachvili, V. Dana, J.-Y. Mandin, Positions and intensities in the 2ν₄/ν₁/ν₃ vibrational system of¹⁴NH₃ near 3 μm //J Mol Spectrosc 193, 46-71 (1999)
10.: Same as I. Kleiner, L.R. Brown, G. Tarrago, Q.-L. Kou, N. Picque, G. Guelachvili, V. Dana, J.-Y. Mandin, Positions and intensities in the 2ν₄/ν₁/ν₃ vibrational system of¹⁴NH₃ near 3 μm // J Mol Spectrosc 193, 46-71 (1999), but upper-state level is unassigned due to mixing from perturbations.
11.: Same as C. Cottaz, I. Kleiner,G. Tarrago, L.R. Brown, J.S. Margolis, P.L. Poynter, H.M. Pickett, T. Fouchet, P. Drossart, Line positions and intensities in the 2ν₂/ν₄ vibrational system of ¹⁴NH₃ near 5–7 μm // J Mol Spectrosc 203, 285-309 (2000), but upper-state level is unassigned due to mixing from perturbations.
12.: K. Sung, L.R. Brown, X. Huang, D.W. Schwenke, T.J. Lee, S.L. Coy, K.K. Lehmann, Extended line positions, intensities, empirical lower state energies and quantum assignments of NH₃ from 6300 to 7000 cm^-1 //JQSRT 113, 1066-1083 (2012)
13.: P. Cacciani, P. Cermak, J. Cosléou, M. Khelkhal, P. Jeseck, X. Michaut, New progress in spectroscopy of ammonia in the infrared 1.5 μm range using evolution of spectra from 300 K down to 122 K //JQSRT 113, 1084-1091 (2012)
14.: M.J. Down, C. Hill, S.N. Yurchenko, J. Tennyson, L.R. Brown, I. Kleiner, Re-analysis of ammonia spectra: Updating the HITRAN ¹⁴NH₃ database //JQSRT 130, 260-272 (2013)