Table 105. H218O (H18OH): Experimental wavenumber, and intensity for the (030)–(010) transitions in the range 2870–3895 cm–1 (Englisch)
Molecular Constants
- Neue Suche nach: Guelachvili, G.
- Neue Suche nach: Picqué, N.
- Neue Suche nach: Guelachvili, G.
- Neue Suche nach: Guelachvili, G.
- Neue Suche nach: Picqué, N.
In:
Non-linear Triatomic Molecules
: Part 1γ
;
387-389
;
2013
- Aufsatz/Kapitel (Buch) / Elektronische Ressource
-
Titel:Table 105. H218O (H18OH): Experimental wavenumber, and intensity for the (030)–(010) transitions in the range 2870–3895 cm–1
-
Untertitel:Molecular Constants
-
Beteiligte:
-
Erschienen in:Non-linear Triatomic Molecules : Part 1γ ; 387-389Landolt-Börnstein - Group II Molecules and Radicals ; 20C1g ; 387-389
-
Verlag:
- Neue Suche nach: Springer Berlin Heidelberg
-
Erscheinungsort:Berlin, Heidelberg
-
Erscheinungsdatum:01.01.2013
-
Format / Umfang:3 pages
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ISBN:
-
ISSN:
-
DOI:
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Medientyp:Aufsatz/Kapitel (Buch)
-
Format:Elektronische Ressource
-
Sprache:Englisch
-
Schlagwörter:
-
Datenquelle:
Inhaltsverzeichnis E-Book
Die Inhaltsverzeichnisse werden automatisch erzeugt und basieren auf den im Index des TIB-Portals verfügbaren Einzelnachweisen der enthaltenen Beiträge. Die Anzeige der Inhaltsverzeichnisse kann daher unvollständig oder lückenhaft sein.
- 1
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IntroductionGuelachvili, G. / Picqué, N. et al. | 2013
- 48
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SurveyGuelachvili, G. / Picqué, N. et al. | 2013
- 77
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Table 1. H217O (H17OH): Rotational and distortion constants for the ground stateGuelachvili, G. / Picqué, N. et al. | 2013
- 78
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Table 2. H217O (H17OH): Ground state rotational constantsGuelachvili, G. / Picqué, N. et al. | 2013
- 80
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Table 3. H217O (H17OH): Molecular parameters for the ground stateGuelachvili, G. / Picqué, N. et al. | 2013
- 81
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Table 4. H217O (H17OH): Molecular parameters for the (000) and the (010) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 82
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Table 5. H217O (H17OH): Molecular parameters for the (020), (100), and the (001) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 83
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Table 6. H217O (H17OH): Fermi and Coriolis coupling constants for the triad {(020), (100), (001)}Guelachvili, G. / Picqué, N. et al. | 2013
- 84
-
Table 7. H217O (H17OH): Molecular constants for the vibrational states (003), (201), (102), (300), (121), (022), (220), (041), (140), and (070) of the first decadeGuelachvili, G. / Picqué, N. et al. | 2013
- 86
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Table 8. H217O (H17OH): Fermi and Coriolis coupling constants for the vibrational states (003), (201), (102), (300), (121), (022), (220), (041), (140), and (070) of the first decadeGuelachvili, G. / Picqué, N. et al. | 2013
- 88
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Table 9. H217O (H17OH): Band origins for 27 vibrational transitionsGuelachvili, G. / Picqué, N. et al. | 2013
- 90
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Table 10. H217O (H17OH): Calculated vibrational band origins for 103 vibrational transitionsGuelachvili, G. / Picqué, N. et al. | 2013
- 93
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Table 11. H217O (H17OH): Force constants for the electronic ground stateGuelachvili, G. / Picqué, N. et al. | 2013
- 96
-
Table 12. H217O (H17OH): Fitted PES parametersGuelachvili, G. / Picqué, N. et al. | 2013
- 99
-
Table 13. H217O (H17OH): Fit coefficients cijk of the morphing functionGuelachvili, G. / Picqué, N. et al. | 2013
- 101
-
Table 14. H217O (H17OH): Force constants of the PES CVRQD calculated at its minimumGuelachvili, G. / Picqué, N. et al. | 2013
- 102
-
Table 15. H217O (H17OH): Dipole moment expansion coefficients for the (000)–(000) and the (010)–(010) bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 103
-
Table 16. H217O (H17OH): Dipole moment expansion coefficients for the (010)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 104
-
Table 17. H217O (H17OH): Dipole moment expansion coefficients for the (100)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 105
-
Table 18. H217O (H17OH): Dipole moment expansion coefficients for the (001)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 106
-
Table 19. H217O (H17OH): Dipole moment expansion effective coefficients for the (020)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 107
-
Table 20. H217O (H17OH): Dipole moment expansion effective coefficients for the (020)–(010) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 108
-
Table 21. H217O (H17OH): Band intensity for 9 vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 109
-
Table 22. H217O (H17OH): Band intensity for the (001)–(000) vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 110
-
Table 23. H217O (H17OH): Band intensity for the (001)–(000), (100)–(000), and (020)–(000) vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 111
-
Table 24. H217O (H17OH): Band intensity for 12 vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 112
-
Table 25. H217O (H17OH): Band intensity for the 3ν polyadGuelachvili, G. / Picqué, N. et al. | 2013
- 113
-
Table 26. H217O (H17OH): Measured frequencies within the vibrational ground state (000), in the range 0.45–177 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 117
-
Table 27. H217O (H17OH): Line position and intensity for the (020)–(020) transitions in the range 51–354 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 120
-
Table 28. H217O (H17OH): Line position and intensity for rotational transitions within the vibrational ground state (000), in the range 53–728 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 129
-
Table 29. H217O (H17OH): Experimental wavenumber, intensity, and shape parameters of rotational transitions within the vibrational ground state (000), in the range 598–797 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 131
-
Table 30. H217O (H17OH): Line position, intensity, and shape parameters for the (010)–(000) transitions in the range 1011–2224 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 146
-
Table 31. H217O (H17OH): Line position, intensity, and shape parameters for the (020)–(010) transitions in the range 1314–1939 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 149
-
Table 32. H217O (H17OH): Line shape related parameters for the (010)–(000) transitions in the range 1371–1735 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 151
-
Table 33. H217O (H17OH): Line position and intensity for the (100)–(010) transitions in the range 1780–2299 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 155
-
Table 34. H217O (H17OH): Line position and intensity for the (001)–(010) transitions in the range 1969–2335 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 159
-
Table 35. H217O (H17OH): Line position and intensity for the (030)–(010) transitions in the range 3405–3886 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 162
-
Table 36. H217O (H17OH): Line position, intensity, and shape parameters for the (020)–(000) transitions in the range 2927–3944 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 168
-
Table 37. H217O (H17OH): Line position, intensity, and shape parameters for the (100)–(000) transitions in the range 3223–4126 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 176
-
Table 38. H217O (H17OH): Line position, intensity, and shape parameters for the (001)–(000) transitions in the range 3225–4242 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 187
-
Table 39. H217O (H17OH): Line position and intensity for the (110)–(010) transitions in the range 3405–3886 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 189
-
Table 40. H217O (H17OH): Line position, intensity, and shape parameters for the (011)–(010) transitions in the range 3591–3857 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 191
-
Table 41. H217O (H17OH): Line position, intensity, and shape parameters for the (001)–(000) transitions in the range 4206–4348 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 193
-
Table 42. H217O (H17OH): Line position, intensity, and shape parameters for the (030)–(000) transitions in the range 4525–5511 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 195
-
Table 43. H217O (H17OH): Line position, intensity, and shape parameters for the (011)–(000) transitions in the range 4778–5953 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 203
-
Table 44. H217O (H17OH): Line position, intensity, and shape parameters for the (011)–(000) transitions in the range 4934–5813 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 206
-
Table 45. H217O (H17OH): Line position, intensity, and shape parameters for the (110)–(000) transitions in the range 4940–5664 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 211
-
Table 46. H217O (H17OH): Line position, intensity, and shape parameters for the (021)–(010) transitions in the range 5101–5371 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 212
-
Table 47. H217O (H17OH): Line position and intensity for the (040)–(000) transitions in the range 5973–6599 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 214
-
Table 48. H218O (H18OH): Rotational and distortion constantsGuelachvili, G. / Picqué, N. et al. | 2013
- 215
-
Table 49. H218O (H18OH): Ground state rotational constantsGuelachvili, G. / Picqué, N. et al. | 2013
- 217
-
Table 50. H218O (H18OH): Molecular parameters for the ground stateGuelachvili, G. / Picqué, N. et al. | 2013
- 218
-
Table 51. H218O (H18OH): Molecular constants for the ground stateGuelachvili, G. / Picqué, N. et al. | 2013
- 220
-
Table 52. H218O (H18OH): Effective and equilibrium ground state rotational constantsGuelachvili, G. / Picqué, N. et al. | 2013
- 222
-
Table 53. H218O (H18OH): Molecular parameters for the (000) and the (010) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 223
-
Table 54. H218O (H18OH): Fitted parameters of the effective Hamiltonian of the (000) and the (010) vibrational statesGuelachvili, G. / Picqué, N. et al. | 2013
- 225
-
Table 55. H218O (H18OH): Molecular constants for the (000) and the (010) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 227
-
Table 56. H218O (H18OH): Molecular parameters for the (020), (100), and the (001) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 228
-
Table 57. H218O (H18OH): Fermi and Coriolis coupling constants for the triad {(020), (100) (001)}Guelachvili, G. / Picqué, N. et al. | 2013
- 229
-
Table 58. H218O (H18OH): Molecular parameters for the (030), (110), and the (011) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 230
-
Table 59. H218O (H18OH): Fermi and Coriolis coupling constants for the triad {(030), (110) (011)}Guelachvili, G. / Picqué, N. et al. | 2013
- 231
-
Table 60. H218O (H18OH): Molecular parameters for the (021), (101), (120), (200), (002), and the (040) statesGuelachvili, G. / Picqué, N. et al. | 2013
- 233
-
Table 61. H218O (H18OH): Coriolis coupling constants for the first hexad {(021), (101), (120), (200), (002), (040)}Guelachvili, G. / Picqué, N. et al. | 2013
- 234
-
Table 62. H218O (H18OH): Fermi coupling constants for the first hexad {(021), (101), (120), (200), (002), (040)}Guelachvili, G. / Picqué, N. et al. | 2013
- 235
-
Table 63. H218O (H18OH): Calculated vibrational band origins for 103 vibrational transitionsGuelachvili, G. / Picqué, N. et al. | 2013
- 238
-
Table 64. H218O (H18OH): Band origins for 39 vibrational transitionsGuelachvili, G. / Picqué, N. et al. | 2013
- 240
-
Table 65. H218O (H18OH): Force constants of the PES CVRQD calculated at its minimumGuelachvili, G. / Picqué, N. et al. | 2013
- 241
-
Table 66. H218O (H18OH): Force constants for the electronic ground stateGuelachvili, G. / Picqué, N. et al. | 2013
- 244
-
Table 67. H218O (H18OH): Fitted PES parametersGuelachvili, G. / Picqué, N. et al. | 2013
- 247
-
Table 68. H218O (H18OH): Fit coefficients cijk of the morphing functionGuelachvili, G. / Picqué, N. et al. | 2013
- 249
-
Table 69. H218O (H18OH): Dipole moment expansion coefficients for the (000)–(000) transitionsGuelachvili, G. / Picqué, N. et al. | 2013
- 250
-
Table 70. H218O (H18OH): Dipole moment expansion coefficients for the (010)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 251
-
Table 71. H218O (H18OH): Dipole moment expansion coefficients for the (100)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 252
-
Table 72. H218O (H18OH): Dipole moment expansion coefficients for the (001)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 253
-
Table 73. H218O (H18OH): Dipole moment expansion effective coefficients for the (020)–(000) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 254
-
Table 74. H218O (H18OH): Dipole moment expansion effective coefficients for the (020)–(010) bandGuelachvili, G. / Picqué, N. et al. | 2013
- 255
-
Table 75. H218O (H18OH): Band intensity for the 3ν polyadGuelachvili, G. / Picqué, N. et al. | 2013
- 256
-
Table 76. H218O (H18OH): Band intensity for 16 vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 257
-
Table 77. H218O (H18OH): Band intensity for the (001)–(000) vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 258
-
Table 78. H218O (H18OH): Band intensity for 15 vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 259
-
Table 79. H218O (H18OH): Band intensity for the (110)–(000), (030)–(000), and (011)–(000) vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 260
-
Table 80. H218O (H18OH): Band intensity for the (101)–(000), (021)–(000), (200)–(000), (002)–(000), (120)–(000), and (040)–(000) vibrational bandsGuelachvili, G. / Picqué, N. et al. | 2013
- 261
-
Table 81. H218O (H18OH): Band intensity for the (131)–(000), (211)–(000), (013)–(000), (230)–(000), (310)–(000), and the (112)–(000) vibrational transitions of the second decadeGuelachvili, G. / Picqué, N. et al. | 2013
- 262
-
Table 82. H218O (H18OH): Band intensity for the (011)–(000) and the (110)–(000) vibrational transitionsGuelachvili, G. / Picqué, N. et al. | 2013
- 263
-
Table 83. H218O (H18OH): Measured frequencies within the vibrational ground state (000), in the range 0.18–208 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 267
-
Table 84. H218O (H18OH): Line position and intensity for rotational transitions within the vibrational ground state (000), in the range 53–725 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 277
-
Table 85. H218O (H18OH): Line position and intensity for the (100)–(100) transitions in the range 53–340 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 280
-
Table 86. H218O (H18OH): Line position and intensity for the (001)–(001) transitions in the range 69–332 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 283
-
Table 87. H218O (H18OH): Experimental wavenumber, and intensity for the (010)–(010) transitions in the range 399–609 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 285
-
Table 88. H218O (H18OH): Experimental wavenumber, and intensity for the (000)–(000) transitions in the range 414–806 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 288
-
Table 89. H218O (H18OH): Calculated wavenumber and intensity of rotational transitions within the vibrational ground state (010), in the range 502–674 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 289
-
Table 90. H218O (H18OH): Experimental wavenumber, intensity, and shape parameters of rotational transitions within the vibrational ground state (000), in the range 595–943 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 292
-
Table 91. H218O (H18OH): Experimental wavenumber, intensity, and line shape parameter for the (010)–(000) transitions in the range 1005–2310 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 317
-
Table 92. H218O (H18OH): Experimental wavenumber, intensity, and line shape parameter of rotational transitions within the vibrational ground state (000), in the range 1009–1193 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 318
-
Table 93. H218O (H18OH): Line position, intensity, and shape parameters for the (010)–(000) transitions in the range 1009–2219 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 336
-
Table 94. H218O (H18OH): Experimental wavenumber, and intensity for the (010)–(000) transitions in the range 1082–2310 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 343
-
Table 95. H218O (H18OH): Experimental wavenumber, and intensity of rotational transitions within the vibrational ground state (000), in the range 1090–1193 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 344
-
Table 96. H218O (H18OH): Experimental wavenumber, and intensity for the (020)–(010) transitions in the range 1104–2091 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 348
-
Table 97. H218O (H18OH): Line position, intensity, and shape parameters for the (020)–(010) transitions in the range 1284–1934 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 353
-
Table 98. H218O (H18OH): Line position and intensity for the (030)–(020) transitions in the range 1290–1856 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 357
-
Table 99. H218O (H18OH): Line shape related parameters for the (010)–(000) transitions in the range 1334–1740 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 360
-
Table 100. H218O (H18OH): Experimental wavenumber, and intensity for the (100)–(010) transitions in the range 1807–2297 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 364
-
Table 101. H218O (H18OH): Experimental wavenumber, intensity, and line shape parameter for the (001)–(010) transitions in the range 1940–2331 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 368
-
Table 102. H218O (H18OH): Experimental wavenumber, and intensity for the (001)–(010) transitions in the range 1950–2474 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 371
-
Table 103. H218O (H18OH): Experimental wavenumber, and intensity for the (001)–(000) transitions in the range 2933–4357 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 380
-
Table 104. H218O (H18OH): Experimental wavenumber, and intensity for the (020)–(000) transitions in the range 2671–4236 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 387
-
Table 105. H218O (H18OH): Experimental wavenumber, and intensity for the (030)–(010) transitions in the range 2870–3895 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 390
-
Table 106. H218O (H18OH): Line position, intensity, and shape parameters for the (020)–(000) transitions in the range 2892–3879 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 398
-
Table 107. H218O (H18OH): Experimental wavenumber, and intensity for the (100)–(000) transitions in the range 2931–4402 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 406
-
Table 108. H218O (H18OH): Line position, intensity, and shape parameters for the (100)–(000) transitions in the range 3117–4152 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 418
-
Table 109. H218O (H18OH): Line position, intensity, and shape parameters for the (001)–(000) transitions in the range 3160–4290 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 431
-
Table 110. H218O (H18OH): Experimental wavenumber, and intensity for the (110)–(010) transitions in the range 3457–4056 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 433
-
Table 111. H218O (H18OH): Experimental wavenumber, and intensity for the (011)–(010) transitions in the range 3351–4099 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 438
-
Table 112. H218O (H18OH): Line position, intensity, and shape parameters for the (001)–(000) transitions in the range 4206–4348 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 441
-
Table 113. H218O (H18OH): Experimental and calculated wavenumber, and intensity for the (030)–(000) transitions in the range 4433–5597 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 446
-
Table 114. H218O (H18OH): Experimental and calculated wavenumber, and intensity for the (110)–(000) transitions in the range 4735–5845 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 458
-
Table 115. H218O (H18OH): Experimental and calculated wavenumber, and intensity for the (011)–(000) transitions in the range 4769–6086 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 476
-
Table 116. H218O (H18OH): Line position, and intensity for the (021)–(010) transitions in the range 4897–5918 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 481
-
Table 117. H218O (H18OH): Experimental wavenumber, and intensity for the (120)–(010) transitions in the range 4956–5509 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 483
-
Table 118. H218O (H18OH): Line position, intensity, and shape parameters for the (021)–(010) transitions in the range 5083–5420 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 485
-
Table 119. H218O (H18OH): Line position and intensity for the (021)–(010) transitions in the range 5915–6087 cm–1Guelachvili, G. / Picqué, N. et al. | 2013
- 486
-
Table 120. H218O (H18OH): Line position and intensity for the (040)–(000) transitions in the range 5924–6999 cm–1Guelachvili, G. / Picqué, N. et al. | 2013