Self-consistent-field calculations on BrCl in a basis of 212 uncontracted Gaussian functions reproduce the measured dipole moment, nuclear quadrupole and spin-rotation coupling constants to within a few percent. The calculated mean polarisability of 36.8 au is 7% smaller than the average of the meas
Electric properties of the ozone molecule
✍ Scribed by K. Andersson; P. Borowski; P.W. Fowler; P.-Å. Malmqvist; B.O. Roos; A.J. Sadlej
- Publisher
- Elsevier Science
- Year
- 1992
- Tongue
- English
- Weight
- 439 KB
- Volume
- 190
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
The dipole moment, quadrupole moment and dipole polarisability of 03 are calculated by the self-consistent field (SCF), many-body perturbation theory (MBPT), complete active space SCF (CASSCF), restricted active space SCF (RASSCF), multireference CI (MRCI) and CASSCF-perturbation theory (CASPT) methods, using a 5s3p2d polarised basis set. At the CASPT-2 level, the dipole moment is #b=0.2136 au. The quadrupole moments are O,~=-1.158, Obb=--0.260, Oct= + 1.418; and the polarisability anisotropies are ct~-abb = 16.2 and aaa-otto= 18.6, all in atomic units. Experimental data for these quantities are 0.2100( I ), -1.03( ), -0.52( ), + 1.55( ), and 19.2(7), 17.9(7), respectively. Similar results are obtained by CASSCF, RASSCF and MRCI, and by MBPT when taken to fourth order. The transverse in-plane polarisability obtained by the singlereference methods shows an erratic behaviour, which is similar to known variations in computed antisymmetric stretching frequencies.
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The quadrupole moment, rotational g factor and magnet&ability tensors of PF, were calculated at the SCF/CHF level in a basis of Gaussian functions, giving values (in au) of &0.561; x1= -17.687; ,Y~ = -14.45 1; g,=O.O719; g, =0.0768 (with the origin at the centre of mass). Electron correlation (estim
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