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HD16O version: IUPAC PART II

Details:

Article: https://doi.org/10.1016/j.jqsrt.2010.06.012
Release date: 2012
Comment: Normal-mode labelling is used for the vibrations, where v1, v2 and v3 stand for the symmetric stretch, bend, and antisymmetric stretch vibrations, respectively. Standard asymmetric-top quantum numbers are used for the rotations, where J, Ka, and Kc are the three quantum numbers associated with rotational angular momentum, J, and the two projections along the A and C axes.

Uploaded Files:

Energy Levels: HD16O_PARTII_EnergyLevels.txt
Transitions: HD16O_PARTII_transitions.txt

References:

TagDOI
00BeNaCahttps://doi.org/10.1006/jmsp.2000.8167
00CaBeNahttps://doi.org/10.1006/jmsp.2000.8192
00NaBeCaSchttps://doi.org/10.1006/jmsp.2000.8087
00NaCahttps://doi.org/10.1006/jmsp.1999.7982
00SiBeMaMahttps://doi.org/10.1006/jmsp.1999.8001
00WaHeHuZhhttps://doi.org/10.1088/0953-2048/14/11/301
01HuHeZhWahttps://doi.org/10.1088/1009-1963/10/11/306
01JeMeCaCohttps://doi.org/10.1006/jmsp.2001.8418
01UlHuBeOnhttps://doi.org/10.1006/jmsp.2001.8382
03BeNaCahttps://doi.org/10.1016/s0022-2852(03)00164-4
03JaTeBeZohttps://doi.org/10.1016/s0022-2852(03)00015-8
04MaRoMiNahttps://doi.org/10.1016/j.jms.2004.05.020
04NaHuHeCahttps://doi.org/10.1039/b312514a
04NaVoHuhttps://doi.org/10.1016/j.jms.2004.06.002
05CaVaNahttps://doi.org/10.1016/j.jms.2005.09.007
05ToNaZoShhttps://doi.org/10.1016/j.jms.2005.05.015
05ToTehttps://doi.org/10.1016/j.jms.2004.12.001
05UlHuBeZhhttps://doi.org/10.1016/j.jms.2005.01.005
06NaLeCahttps://doi.org/10.1016/j.jms.2005.12.008
07JeDaReTyhttps://doi.org/10.1016/j.jqsrt.2006.11.007
07MaToCahttps://doi.org/10.1016/j.jms.2007.02.020
07MiWaKaCahttps://doi.org/10.1016/j.jms.2007.05.013
07VoNaCaCohttps://doi.org/10.1016/j.jms.2007.03.008
08LiHohttps://doi.org/10.1016/j.jms.2007.12.007
08NaVoMaTehttps://doi.org/10.1016/j.jms.2007.12.005
08PeSoSihttps://doi.org/10.1117/12.783034
08ToTehttps://doi.org/10.1016/j.jqsrt.2007.08.001
09LiNaKaCahttps://doi.org/10.1016/j.jqsrt.2009.04.013
10NaBeLeCahttps://doi.org/10.1016/j.jqsrt.2009.06.016
46ToMehttps://doi.org/10.1103/physrev.70.558
49Mcafee-
49Strandbehttps://doi.org/10.1063/1.1747084
53BeWehttps://doi.org/10.1103/physrev.91.1014
53Crawfordhttps://doi.org/10.1063/1.1698790
53JeBiMahttps://doi.org/10.1063/1.1698937
54PoSthttps://doi.org/10.1103/physrev.95.374
55WeBeHehttps://doi.org/10.1063/1.1742394
56ErCohttps://doi.org/10.1063/1.1743051
57Posenerhttps://doi.org/10.1071/ph570276
62TrBehttps://doi.org/10.1063/1.1732766
64ThKrLohttps://doi.org/10.1063/1.1725107
67BlVeDyhttps://doi.org/10.1016/0375-9601(67)90864-x
68VeBlDyhttps://doi.org/10.1016/0375-9601(68)90256-9
70BeSt-
70StBe-
71DeCoHeGohttps://doi.org/10.1063/1.1675675
71LaBeSt-
73CaFlGuAmhttps://doi.org/10.1080/00268977300102131
73ClBeKlRohttps://doi.org/10.1063/1.1680328
76FlGihttps://doi.org/10.1016/0022-2852(76)90273-3
78KaKaKyhttps://doi.org/10.1016/0022-2852(78)90073-5
82PaCaFlGuhttps://doi.org/10.1016/0022-2852(82)90115-1
82ToGuBrhttps://doi.org/10.1364/ao.21.003337
83Guelachvhttps://doi.org/10.1364/josa.73.000137
83ToBrhttps://doi.org/10.1364/ao.22.000908
84MeDeHehttps://doi.org/10.1016/0022-2852(84)90109-7
85Johnshttps://doi.org/10.1364/josab.2.001340
86FlCaMaGuhttps://doi.org/10.1007/bf01026692
87BaAlAlPo-
89OhSahttps://doi.org/10.1016/0022-2852(89)90335-4
90ByKaKoNa-
91RiSmDeBehttps://doi.org/10.1016/0022-2852(91)90255-9
91SaTaIrNahttps://doi.org/10.1364/josab.8.000713
92RiSmDeBehttps://doi.org/10.1016/0022-2852(92)90251-i
93GoFeDeDuhttps://doi.org/10.1006/jmsp.1993.1292
93Tothbhttps://doi.org/10.1006/jmsp.1993.1266
95PaHohttps://doi.org/10.1364/josab.12.001813
97Tothbhttps://doi.org/10.1006/jmsp.1997.7451
97Tothchttps://doi.org/10.1006/jmsp.1997.7398
97VoFaPlRihttps://doi.org/10.1063/1.475177
98LaPeSiZh-
99HuLiHeChhttps://doi.org/10.1039/a903593a
99NaBeCahttps://doi.org/10.1006/jmsp.1999.7917
99Tothhttps://doi.org/10.1006/jmsp.1999.7814

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