<p><p>With the development of modern instruments and theories, a considerable amount of spectroscopic informationis being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data ar
Non-linear Triatomic Molecules: Part 1Ξ²
β Scribed by G. Guelachvili (eds.)
- Publisher
- Springer-Verlag Berlin Heidelberg
- Year
- 2012
- Tongue
- English
- Leaves
- 480
- Series
- Landolt-BΓΆrnstein - Group II Molecules and Radicals 20C1b
- Edition
- 1
- Category
- Library
No coin nor oath required. For personal study only.
β¦ Synopsis
With the development of modern instruments and theories, a considerable amount of spectroscopic informationis being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data are measured often with extreme sensitivity. These data are also analyzed and precise molecular parameters determined. Volume II/20, βMolecular Constants Mostly from Infrared Spectroscopyβ, is a recent Landolt-BΓΆrnstein publication series bringing together these results. It is made up of several volumes (A, B, C, D) with comprehensive compilation of critically evaluated molecular constants of diatomic (A), linear triatomic (B); nonlinear triatomic (C), and other polyatomic (D) molecules. Subvolume II/20C1 is devoted to H2O.
β¦ Table of Contents
Preface
Contents
A Introduction
I Energy level designations
I.1 Vibrational assignment
I.1.1 Normal and local modes
I.1.1.1 Normal modes
I.1.1.2 Local modes
I.1.2 Polyads
I.1.3 Vibrational interactions
I.2 Rotational assignment
I.3 Ortho-para transitions
II Energy expressions referred to the ground state
II.1 Vibrational states
II.2 Simple expressions for the fundamental frequencies
III Effective Hamiltonians
III.1 A-reduced Watson-type rotational Hamiltonian
III.2 Coudert Hamiltonian with Radauβs coordinates
III.3 Tyuterev Hamiltonian with Generating Function Model
IV Perturbation-theory free Hamiltonians
IV.1 Jensen Morse Oscillator-Rigid Bender Internal Dynamics Hamiltonian
IV.2 Vibrational Hamiltonian expanded in terms of local Morse operators
V Potential energy
V.1 Potential Energy Function (PEF) expanded as a power series
V.2 Spectroscopically determined Potential Energy Surface (PES)
V.2.1 Jensenβs PES determined by variational calculation of rotation-vibration energies with MORBID Hamiltonian
V.2.2 Effective isotope-independent Born-Oppenheimer (B-O) PES with isotope-dependent adiabatic correction
V.2.3 Isotope-dependent PES from high-quality ab-initio analytical potential representation
V.2.4 Semitheoretical PES by morphing ab-initio potential
V.2.5 Correction to the ab-initio PES expression from [2000Kai] for the determination of the barrier height
V.2.6 Force constants
VI Dipole moment function (DMF)
VI.1 One example of a Taylor series expansion form of the DMF
VI.2 DMF expression in [97Cou]
VI.3 Analytical expression of the Dipole Moment Surface in [97Par]
VI.4 Dipole matrix elements in the DMS expansion used in [2005Tot2]
VI.5 Transition moment for the bending-rotation Coudert Hamiltonian approach
VII Intensities
VII.1 Line intensity
VII.2 Band intensity
VII.3 Temperature dependence of the absorption
VII.4 Internal partition function
VIII Line shape
VIII.1 Line profiles
VIII.1.1 Lorentz profile
VIII.1.2 Doppler profile
VIII.1.3 Voigt profile
VIII.2 Collision-broadening
VIII.2.1 Self-broadening
VIII.2.2 Foreign gas broadening
VIII.2.3 Temperature dependence of the line broadening coefficients
VIII.3 Family of H2O lines
IX Conversion tables
IX.1 Conversion table for energy-related units and selected fundamental constants
IX.2 Intensity units and conversion table
X List of symbols
References
XI Survey
XI.1. Band intensities
XI.2. Band origins
XI.3. Barrier to linearity
XI.4. Difference bands
XI.5. Dipole moments
XI.6. Dissociation energy
XI.7. Energy levels
XI.8. Force constants
XI.9. Hamiltonian parameters
XI.10. Harmonic frequencies
XI.11. Line positions with relative intensities
XI.12. Line positions with line intensity unit
XI.13. Line shape related parameters
XI.14. Morphing function
XI.15. Partition function
XI.16. Potential
XI.17. Spectroscopic parameters
XI.18. Structure
XI.19. Temperature-dependent absorption coefficient
XI Detailed survey of some tables
B Data
1 H2O (HOH) cont.
1.1 H216O (H16OH) cont.
Table 163. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(020)β(010) vibrational band, in the range 943β2482 cmβ1.
References
Table 164. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(040)β(030) vibrational band, in the range 949β2427 cmβ1.
Reference
Table 165. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (030)β(020) vibrational band, in the range 968β2488 cmβ1.
Reference
Table 166. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (010)β(000)vibrational band, in the range 973β2041 cmβ1.
Reference
Table 167. H216O(H16OH): Wavenumbers and intensities for rovibrational transitions belonging to the (010)β(000) vibrational band, in the range 977β2500 cmβ1.
Reference
Table 168. H216O(H16OH): Line position and intensity for the rovibrational transitions (020)β(010) in therange 995β2154 cmβ1.
References
Table 169. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(001) vibrational band, in the range 1008β1991 cmβ1.
Reference
Table 170. H216O(H16OH): Wavenumbers, intensities, and self-broadening coefficients of rovibrationaltransitions belonging to the (010)β(000) vibrational band, in the range1014β1063 cmβ1.
Reference
Table 171. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (100)β(010) vibrational band, in the range 1031β1899 cmβ1.
References
Table 172. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (110)β(100) vibrational band, in the range 1040β1986 cmβ1.
Reference
Table 173. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (030)β(020) vibrational band, in the range 1042β2242 cmβ1.
Reference
Table 174. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (001)β(010) vibrational band, in the range 1051β1942 cmβ1.
Reference
Table 175. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (100)β(010) vibrational band, in the range 1086β2499 cmβ1.
Reference
Table 176. H216O(H16OH): Collisional half-widths of rovibrational transitions belonging to the (040)β(030) band.
Reference
Table 177. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (110)β(100) vibrational band, in the range 1104β2376 cmβ1.
Reference
Table 178. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (001)β(010) vibrational band, in the range 1104β2499 cmβ1.
Reference
Table 179. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(001) vibrational band, in the range 1116β2328 cmβ1.
Reference
Table 180. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (040)β(030) vibrational band, in the range 1126β1647 cmβ1.
Reference
Table 181. H216O(H16OH): Collisional half-widths of rovibrational transitions belonging to the (020)β(010) band.
Reference
Table 182. H216O(H16OH): Collisional half-widths of rovibrational transitions belonging to the (011)β(001), (110)β(100), (100)β(010), (021)β(011) bands.
Reference
Table 183. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (020)β(000) vibrational band, in the range 1194β1664 cmβ1.
Reference
Table 184. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(020) vibrational band, in the range 1212β1992 cmβ1.
Reference
Table 185. H216O(H16OH): Collisional half-widths of rovibrational transitions belonging to the (030)β(020) band.
Reference
Table 186. H216O(H16OH): Line position and intensity for the rovibrational transitions (100)β(010) in therange 1247β2423 cmβ1.
References
Table 187. H216O(H16OH): Wavenumbers and intensities for rovibrational transitions belonging to the (010)β(000) vibrational band, in the range 1258β1749 cmβ1.
Reference
Table 188. H216O(H16OH): Self- and Nitrogenβbroadening coefficients for rovibrational transitionsbelonging to the (010)β(000) vibrational band, in the range 1598β1516 cmβ1.
References
Table 189. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (010)β(000) vibrational band, in the range 1500β1524 cmβ1.
References
Table 190. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(020) vibrational band, in the range 1845β2491 cmβ1.
Reference
Table 191. H216O(H16OH): Observed line position and intensity for rovibrational transitions belonging tothe (100)β(010) vibrational band, in the range 1871β2394 cmβ1.
Reference
Table 192. H216O(H16OH): Line position and intensity for the rovibrational transitions (001)β(010) in therange 1876β2572 cmβ1.
References
Table 193. H216O(
H16OH): Line position and intensity for rovibrational transitions belonging to the (110)β(100) vibrational band, in the range 2004β2453 cmβ1.
Reference
Table 194. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (030)β(020) vibrational band, in the range 2004β2756 cmβ1.
Reference
Table 195. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(020) vibrational band, in the range 2004β4078 cmβ1.
Reference
Table 196. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(001) vibrational band, in the range 2010β2424 cmβ1.
Reference
Table 197. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (100)β(010) vibrational band, in the range 2014β2564 cmβ1.
Reference
Table 198. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (100)β(000) vibrational band, in the range 2014β4717 cmβ1.
Reference
Table 199. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (001)β(010) vibrational band, in the range 2017β4091 cmβ1.
Reference
Table 200. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (040)β(030) vibrational band, in the range 2026β2440 cmβ1.
Reference
Table 201. H216O(H16OH): Measured intensities versus temperature for two doublets of the (010)β(000) band respectively located at 2136 and 2115 cmβ1.
References
Table 202. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(010) vibrational band, in the range 2405β4715 cmβ1.
Reference
Table 203. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (110)β(010) vibrational band, in the range 2477β4730 cmβ1.
Reference
Table 204. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (100)β(000) vibrational band, in the range 2499β3195 cmβ1.
Reference
Table 205. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (001)β(000) vibrational band, in the range 2501β3195 cmβ1.
Reference
Table 206. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(021)β(020) vibrational band, in the range 2503β4742 cmβ1.
Reference
Table 207. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(020)β(000) vibrational band, in the range 2534β4574 cmβ1.
Reference
Table 208. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(030)β(010) vibrational band, in the range 2553β4375 cmβ1.
Reference
Table 209. H216O(H16OH): Line position and intensity for the rovibrational transitions (020)β(000) in therange 2622β4261 cmβ1.
References
Table 210. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (020)β(000)vibrational band, in the range 2661β4234 cmβ1.
Reference
Table 211. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (011)β(010)vibrational band, in the range 2679β4245 cmβ1.
Reference
Table 212. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (001)β(000)vibrational band, in the range 2731β4193 cmβ1.
Reference
Table 213. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (030)β(010)vibrational band, in the range 2746β3195 cmβ1.
Reference
Table 214. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(030)β(000) vibrational band, in the range 2756β4274 cmβ1.
Reference
Table 215. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (110)β(010)vibrational band, in the range 2789β4216 cmβ1.
Reference
Table 216. H216O(H16OH): Experimental positions and intensities for rovibrational transitions belongingto the (100)β(000) vibrational band, in the range 2912β4469 cmβ1.
References
Table 217. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(030)β(010) vibrational band, in the range 2926β3375 cmβ1.
Reference
Table 218. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(001)β(000) vibrational band, in the range 2972β4231 cmβ1.
Reference
Table 219. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(001)β(000) vibrational band, in the range 2992β4506 cmβ1.
References
Table 220. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the(011)β(000) vibrational band, in the range 3005β4742 cmβ1.
Reference
Table 221. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (020)β(000) vibrational band, in the range 3010β3898 cmβ1.
Reference
Table 222. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (100)β(000) vibrational band, in the range 3310β3995 cmβ1.
Reference
Table 223. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (110)β(010) vibrational band, in the range 3325β3927 cmβ1.
Reference
Table 224. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (001)β(000) vibrational band, in the range 3355β4045 cmβ1.
Reference
Table 225. H2 6O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(010) vibrational band, in the range 3381β4114 cmβ1.
Reference
Table 226. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (021)β(020) vibrational band, in the range 3533β3635 cmβ1.
Reference
Table 227. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (001)β(000) vibrational band, in the range 4200β4496 cmβ1.
Reference
Table 228. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (100)β(000) vibrational band, in the range 4200β4496 cmβ1.
Reference
Table 229. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (020)β(000) vibrational band, in the range 4212β4402 cmβ1.
Reference
Table 230. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (030)β(000) vibrational band, in the range 4359β4996 cmβ1.
Reference
Table 231. H216O(H16OH): Line position intensity and selfβbroadened width coefficient for rovibrational transitions belonging to the (030)β(000) vibrational band, in the range 4450β 4986 cmβ1.
Reference
Table 232. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (110)β(000) vibrational band, in the range 4568β4997 cmβ1.
Reference
Table 233. H216O(H16OH): Line position and intensity for rovibrational transitions belonging to the (011)β(000) vibrational band, in the range 4608β4999 cmβ1.
Reference
Table 234. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (021)β(010) vibrational band, in the range 4751β4993 cmβ1.
References
Table 235. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (011)β(000) vibrational band, in the range 4754β5000 cmβ1.
References
Table 236. H216O(H16OH): Line position intensity and self-broadened width coefficient for rovibrational transitions belonging to the (110)β(000) vibrational band, in the range 4761β4997 cmβ1.
Reference
Table 237. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (001)β(000) vibrational band, in the range 4762β5004 cmβ1.
References
Table 238. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (110)β(000) vibrational band, in the range 4764β4968 cmβ1.
References
Table 239. H216O(H16OH): Line position intensity and self-broadened width coefficient for rovibrational transitions belonging to the (011)β(000) vibrational band, in the range 4787β4998 cmβ1.
Reference
Table 240. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (011)β(000) vibrational band, in the range 4788β4988 cmβ1.
References
Table 241. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (030)β(000) vibrational band, in the range 4847β4998 cmβ1.
References
Table 242. H216O(H16OH): Line parameters for rovibrational transitions belonging to the (021)β(010) vibrational band, in the range 4878β4994 cmβ1.
References
π SIMILAR VOLUMES
<p><p>With the development of modern instruments and theories, a considerable amount of spectroscopic informationis being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data ar
<p><p>With the development of modern instruments and theories, a considerable amount of spectroscopic informationis being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data ar
<p><p>With the development of modern instruments and theories, a considerable amount of spectroscopic information is being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data a
<p><p>With the development of modern instruments and theories, a considerable amount of spectroscopic informationis being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data ar
<p><p>With the development of modern instruments and theories, a considerable amount of spectroscopic information is being permanently collected on molecules. The infrared, in particular, is seeing extraordinary activities. Using Fourier transform interferometers and infrared lasers, accurate data a