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Subject Index for Volume 214
Journal of Molecular Spectroscopy 214, 230 (2002) doi:10.1006/jmsp.2002.8658
Subject Index for Volume 214 A Ab initio studies CHCl2 OH, MRD-CI calculations of excited electronic states, Schnell, M¨uhlh¨auser, and Peyerimhoff, 124 Axis switching relationship to Coriolis coupling in the spectra of HCCl and DCCl, Lin et al., 216
L Lineshape studies confinement narrowing of 13 CO, (1,0), R(0) line by He, Henry et al., 28 M MgO transition probabilities for B 1 + –X 1 + , A1 systems, Daily et al., 111
B
P
B2 calculation of (1–3)3 g rotational levels, complex scaled finite element method, Andersson, Pederson, and Elander, 103
Pressure broadening studies N2 H4 , ν12 , Plunkett et al., Vol. 211, pg. 241; erratum, 227 R
E Electronic spectra 13 C16 O+ , A2 , v = 1–5 –X 2 + (Comet tail) system, emission, K¸ epa et al., i 117 C5 H4 OS (4H-pyran-4-thione), T1 ← S0 system (594 nm), cavity ringdown, Ruth et al., 80 DCCl, A˜ 1 A – X˜ 1 A , 210 band (774 nm), molecular structure and axisswitching effects, Lin et al., 216 HC4 D+ (diacetylene-d1 cation), A2 –X 2 , (0,0) band (507 nm), rotational analysis, Vaizert et al., 94 IBr, A3 1 ← X 1 + , 11330–13220 cm−1 , Yukiya, Nishimiya, and Suzuki, 132 NiF, reanalysis of visible region FT emission, new 1/2 state at 20106 cm−1 , Krouti et al., 152 TiO, B 3 –X 3 (1,0) band (584 nm), isotope shift, Amiot, Luc, and Vetter, 196 electronic transition moment function, Namiki and Ito, 188
Rotational spectra (CO)2 (carbon monoxide dimer), 60–176 GHz, 14 new levels in three new vibrational states, possibility of isomerism, Tang et al., 87 C4 H10 O–Ar (butan-2-ol–argon complex), 6–16 GHz, King and Howard, 97 C6 H5 ClO (cis-2-chlorophenol, Cl-C6 H4 -OH), 5–12 GHz, quadrupole coupling, Onda et al., 129 Rg · ND3 complexes (Rg = Ne, Kr), 10 –00 hindered rotational band, 195–298 GHz, Melnik, Miller, and De Lucia, 202 T Tetra-atomic molecules a generational method for calculating vibrational energy levels, Yu and Muckerman, 11 Torsion in methyl top molecules internal rotation angle, definition and variation of small amplitude frequencies with, Xu et al., 175 V
H
Vibration–rotation spectra CH3 CF3 , 510 (610 cm−1 ) and 510 611 bands, Wang et al., 69 C2 H6 , combined fit to ν3 (994 cm−1 ), ν9 (974 cm−1 ) and 3ν4 , reassessment of the torsional potential, Moazzen-Ahmadi, 144 D3 SiF, 11 , 41 , 21 31 , 31 51 polyad (1578, 1615, 1604, 1590 cm−1 ), Boulaftali et al., 35 OH, revised constants for X 2 , v = 0–10, Colin et al., 225 PHD2 , ν3 , ν4 , ν6 (912, 767, 979 cm−1 ), Ulenikov et al., 1 SF4 , ν1 (892 cm−1 ), Raffael and Smith, 21
H2 O vibron model approximation for vibrational level energies to 18000 cm−1 , Lemus et al., 52 I Intensity studies N2 H4 , ν12 , Plunkett et al., Vol. 211, pg. 241; erratum, 227
0022-2852/02 $35.00 C 2002 Elsevier Science (USA) All rights reserved.
230
Subject Index for Volume 214 A Ab initio studies CHCl2 OH, MRD-CI calculations of excited electronic states, Schnell, M¨uhlh¨auser, and Peyerimhoff, 124 Axis switching relationship to Coriolis coupling in the spectra of HCCl and DCCl, Lin et al., 216
L Lineshape studies confinement narrowing of 13 CO, (1,0), R(0) line by He, Henry et al., 28 M MgO transition probabilities for B 1 + –X 1 + , A1 systems, Daily et al., 111
B
P
B2 calculation of (1–3)3 g rotational levels, complex scaled finite element method, Andersson, Pederson, and Elander, 103
Pressure broadening studies N2 H4 , ν12 , Plunkett et al., Vol. 211, pg. 241; erratum, 227 R
E Electronic spectra 13 C16 O+ , A2 , v = 1–5 –X 2 + (Comet tail) system, emission, K¸ epa et al., i 117 C5 H4 OS (4H-pyran-4-thione), T1 ← S0 system (594 nm), cavity ringdown, Ruth et al., 80 DCCl, A˜ 1 A – X˜ 1 A , 210 band (774 nm), molecular structure and axisswitching effects, Lin et al., 216 HC4 D+ (diacetylene-d1 cation), A2 –X 2 , (0,0) band (507 nm), rotational analysis, Vaizert et al., 94 IBr, A3 1 ← X 1 + , 11330–13220 cm−1 , Yukiya, Nishimiya, and Suzuki, 132 NiF, reanalysis of visible region FT emission, new 1/2 state at 20106 cm−1 , Krouti et al., 152 TiO, B 3 –X 3 (1,0) band (584 nm), isotope shift, Amiot, Luc, and Vetter, 196 electronic transition moment function, Namiki and Ito, 188
Rotational spectra (CO)2 (carbon monoxide dimer), 60–176 GHz, 14 new levels in three new vibrational states, possibility of isomerism, Tang et al., 87 C4 H10 O–Ar (butan-2-ol–argon complex), 6–16 GHz, King and Howard, 97 C6 H5 ClO (cis-2-chlorophenol, Cl-C6 H4 -OH), 5–12 GHz, quadrupole coupling, Onda et al., 129 Rg · ND3 complexes (Rg = Ne, Kr), 10 –00 hindered rotational band, 195–298 GHz, Melnik, Miller, and De Lucia, 202 T Tetra-atomic molecules a generational method for calculating vibrational energy levels, Yu and Muckerman, 11 Torsion in methyl top molecules internal rotation angle, definition and variation of small amplitude frequencies with, Xu et al., 175 V
H
Vibration–rotation spectra CH3 CF3 , 510 (610 cm−1 ) and 510 611 bands, Wang et al., 69 C2 H6 , combined fit to ν3 (994 cm−1 ), ν9 (974 cm−1 ) and 3ν4 , reassessment of the torsional potential, Moazzen-Ahmadi, 144 D3 SiF, 11 , 41 , 21 31 , 31 51 polyad (1578, 1615, 1604, 1590 cm−1 ), Boulaftali et al., 35 OH, revised constants for X 2 , v = 0–10, Colin et al., 225 PHD2 , ν3 , ν4 , ν6 (912, 767, 979 cm−1 ), Ulenikov et al., 1 SF4 , ν1 (892 cm−1 ), Raffael and Smith, 21
H2 O vibron model approximation for vibrational level energies to 18000 cm−1 , Lemus et al., 52 I Intensity studies N2 H4 , ν12 , Plunkett et al., Vol. 211, pg. 241; erratum, 227
0022-2852/02 $35.00 C 2002 Elsevier Science (USA) All rights reserved.
230