1983
DOI: 10.1007/bf01204322
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Electron paramagnetic resonance of PO 3 2? and SO 3 ? radicals in anhydrite, celestite and barite: the hyperfine structure and dynamics

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Cited by 28 publications
(12 citation statements)
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“…Their concentration turns out to be small and near to that of the corresponding isoelectronic 33SO;-and 33SO2 radicals containing the rare isotope 33S with natural abundance 0.75% (see, for example, EPR spectrum in Fig. 2 in the work of Ryabov et al 1983). As an exception, one of the two PO~-radicals in CaSO4 showed a concentration more than 10-fold higher.…”
Section: Introductionmentioning
confidence: 82%
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“…Their concentration turns out to be small and near to that of the corresponding isoelectronic 33SO;-and 33SO2 radicals containing the rare isotope 33S with natural abundance 0.75% (see, for example, EPR spectrum in Fig. 2 in the work of Ryabov et al 1983). As an exception, one of the two PO~-radicals in CaSO4 showed a concentration more than 10-fold higher.…”
Section: Introductionmentioning
confidence: 82%
“…In celestite and barite the multiplicity was KM= 2; g and A tensors have only one coinciding principal axis parallel to the crystallographic axis b. As follows from Table 4 of Ryabov et al (1983), such values of K ~t and directions of the principal axes of the g and A tensors are inherent in paramagnetic centers localized in c position with point group 2 mm (the number of the translationally inequivalent points in the unit cell is K~ = 2) in space group Aroma for anhydrite, and in c position with point group m (K~--4) in space group Pnma for celestite and barite. The point group of the SO4 tetrahedra is just the same, i.e.…”
Section: Identification Of Paramagnetic Centermentioning
confidence: 95%
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“…The point symmetry of the SO~-and PO~-radicals in barite is m. Therefore, for them as well as for the SO3 radical (Ryabov et al 1983) a low symmetry effect is observed implying a noncoincidence of the principal axes of the g-and A-tensors in the ac plane. For the PO22-radical (where the angle between z and z' axes equals to 12 ~ this effect is more pronounced than for the SO~ radical (5~ Schneider et al (1966) were able to determine the signs of the HFI constants of the SOy radical in KC1 by averaging the dipole-dipole electron-nuclear interaction to zero at the room temperature.…”
Section: Model Of Po~-and So; Centersmentioning
confidence: 88%