Abstract:Spectroscopic properties of dimers, hydrides, oxides, fluorides and sulphides of the elements In, Sn and Sb have been calculated using energy-adjusted pseudopotentials. Results are given for bond lengths R e, dissociation energies D e, vibrational frequencies co e and dipole moments #e of the ground states.Comparison is made both with experimental and theoretical values, where available.
“…Froben et al, 15 on the basis of Raman spectra of matrix-isolated group IIIA dimers, reported a 3 ⌺ Ϫ ground state and e ϭ118 cm Ϫ1 and as a consequence the dissociation energy quoted by Huber and Herzberg 4 (1.0 1 eV) was corrected to 0.87 eV or 84 kJ mol Ϫ1 . More recently, the theoretical investigations carried out by Balasubramanian and Li 10 and Igel-Mann et al 11 agree, as mentioned above, in quoting a 3 ⌸ ground state and in the corresponding D e values ͑1.02 and 1.09 eV, respectively͒. Balasubramanian and Li, 10 on the other hand, found the spin-orbit effect to be non-negligible for the electronic states of In 2 .…”
Section: B Insupporting
confidence: 49%
“…Both the two theoretical investigations carried out by Balasubramanian and Li 10 and Igel-Mann et al 11 agree in finding the 3 ⌸ state to be the ground state for In 2 . In the evaluation of the thermal functions we utilized the relativistic results of Balasubramanian and Li 10 where the electronic levels including the -coupling are provided.…”
The group III metal dimers Ga2 and In2 and the newly identified intermetallic molecule GaIn were investigated in a Knudsen cell-mass spectrometric study of the vapors over gallium–indium alloys. From the all-gas equilibria analyzed by the second-law and third-law methods the following dissociation energies were derived; D00 (Ga2)=110.8±4.9 kJ mol−1, D00 (In2)=74.4±5.7 kJ mol−1, D00 (GaIn)=90.7±3.7 kJ mol−1. The value here measured for the dissociation energy of In2 is discussed and compared with a previous experimental determination and with the results of more recent theoretical investigations.
“…Froben et al, 15 on the basis of Raman spectra of matrix-isolated group IIIA dimers, reported a 3 ⌺ Ϫ ground state and e ϭ118 cm Ϫ1 and as a consequence the dissociation energy quoted by Huber and Herzberg 4 (1.0 1 eV) was corrected to 0.87 eV or 84 kJ mol Ϫ1 . More recently, the theoretical investigations carried out by Balasubramanian and Li 10 and Igel-Mann et al 11 agree, as mentioned above, in quoting a 3 ⌸ ground state and in the corresponding D e values ͑1.02 and 1.09 eV, respectively͒. Balasubramanian and Li, 10 on the other hand, found the spin-orbit effect to be non-negligible for the electronic states of In 2 .…”
Section: B Insupporting
confidence: 49%
“…Both the two theoretical investigations carried out by Balasubramanian and Li 10 and Igel-Mann et al 11 agree in finding the 3 ⌸ state to be the ground state for In 2 . In the evaluation of the thermal functions we utilized the relativistic results of Balasubramanian and Li 10 where the electronic levels including the -coupling are provided.…”
The group III metal dimers Ga2 and In2 and the newly identified intermetallic molecule GaIn were investigated in a Knudsen cell-mass spectrometric study of the vapors over gallium–indium alloys. From the all-gas equilibria analyzed by the second-law and third-law methods the following dissociation energies were derived; D00 (Ga2)=110.8±4.9 kJ mol−1, D00 (In2)=74.4±5.7 kJ mol−1, D00 (GaIn)=90.7±3.7 kJ mol−1. The value here measured for the dissociation energy of In2 is discussed and compared with a previous experimental determination and with the results of more recent theoretical investigations.
“…The inaccuracy of bond lengths and bond angles due to that treatment is expected to be small as demonstrated for related compounds in several earlier papers [41][42][43]. The equilibrium structures are found to be three-dimensional geometries for m >/4, i.e., a tetrahedron for m = 4, a square pyramid for m = 5 and a trigonal prisma for m = 6.…”
Section: Discussionmentioning
confidence: 93%
“…For this geometry, calculations including valance correlation were performed for the neutral Xm cluster and the singly charged ions Xm + in order to determine the atomization energies (De) and the (vertical) ionization potentials (IP). (It has been shown in recent papers [41][42][43] that there is no qualitative change in geometry between SCF and the valencecorrelated level.) In the case of the dimers )(2, additionally, vibrational frequencies to e were determined by calculating (total) valence energies at four or five points around the minimum of the potential curve (with AR e = 0-1 a0) and fitting these values to third-degree polynomials at each level of approximation.…”
Homonuclear clusters X m of heavy group V atoms (X = As, Sb) up to m = 6 have been studied with valence ab initio self consistent field/configuration integration calculations using energy-adjusted pseudopotentials. Several structures have been investigated and results are given for bond lengths (Re) , atomization energies (De) and vertical ionization potentials of the ground states. Comparison with experimental and other theoretical values is made where possible.
“…In fact, such calculations have been reported in some of the abovementioned mass spectrometric studies. 3,5 In addition, DFT and/or ab initio calculations have been performed in other spectroscopic studies of various antimony oxides in order to assist spectral assignments, 9,15 and there are also numerous independent computational studies on antimony oxides, [16][17][18][19][20][21][22] though most of these computational studies are on the diatomic antimony monoxide SbO. [16][17][18][19][20][21] To our knowledge, however, there are only two computational studies, which have considered the triatomic antimony dioxide ͑SbO 2 ͒.…”
Geometry optimization and harmonic vibrational frequency calculations have been carried out on the low-lying doublet electronic states of antimony dioxide ͑SbO 2 ͒ employing a variety of ab initio methods, including the complete active space self-consistent field/multireference configuration interaction and the RCCSD͑T͒ methods. Both large and small core relativistic effective core potentials were used for Sb in these calculations, together with valence basis sets of up to aug-cc-pV5Z quality. Contributions from outer core correlation and off-diagonal spin-orbit interaction to relative electronic energies have been calculated. The ground electronic state of SbO 2 is determined to be the X 2 A 1 state, as is the case for dioxides of other lighter group 15 p-block ͑or group VA͒ elements. However, the à 2 B 2 and B 2 A 2 states are estimated to be only 4.1 and 10.7 kcal/ mole above the X 2 A 1 state, respectively, at the complete basis set limit. Reliable vertical excitation energies from the X 2 A 1 state to low-lying excited states of SbO 2 have been computed with a view to assist future spectral assignments of the absorption and/or laser-induced fluorescence spectra of SbO 2 , when they become available.
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