1990
DOI: 10.1021/ic00336a018
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EPR and ENDOR spectra of copper(II) centers with dz2 and dx2-y2 ground states in barium hexafluorozincate: analysis of hyperfine parameters and dynamic vibronic coupling

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Cited by 41 publications
(49 citation statements)
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“…It contributes to stabilizing the elongated with respect to the compressed D 4h conformation [10], because in the former case two electrons are lowered in energy instead of only one in the latter case. The e ds /e s ratio for the planar Cu II O 4 coordination (in Li 2 CuO 2 ) [11] and for the planar CuCl 4 2-complex [12] is found to be similar to the value above (@0.26), while it is much smaller in the case of the ionic F -ligand (≈0.07: Cu II F 4 square plane in BaCuF 4 [13]). In the CuCl 4 2-case it is remarkable that the AOM parameters are well transferable from the planar to the (D 2d -distorted) tetrahedral coordination [10].…”
Section: D-s Mixing In the Aomsupporting
confidence: 65%
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“…It contributes to stabilizing the elongated with respect to the compressed D 4h conformation [10], because in the former case two electrons are lowered in energy instead of only one in the latter case. The e ds /e s ratio for the planar Cu II O 4 coordination (in Li 2 CuO 2 ) [11] and for the planar CuCl 4 2-complex [12] is found to be similar to the value above (@0.26), while it is much smaller in the case of the ionic F -ligand (≈0.07: Cu II F 4 square plane in BaCuF 4 [13]). In the CuCl 4 2-case it is remarkable that the AOM parameters are well transferable from the planar to the (D 2d -distorted) tetrahedral coordination [10].…”
Section: D-s Mixing In the Aomsupporting
confidence: 65%
“…1). The hyperfine interaction with the copper nucleus, particularly the isotropic contribution, is extremely sensitive to s-admixing -here induced by the a 1g *(3d z2 )-a 1g *(4s) pseudo Jahn-Teller interaction -because this implies a small unpaired electron density directly at the copper nucleus via the 1s orbital [13].…”
Section: D-s Mixing In the Aommentioning
confidence: 99%
“…The value is close to the observed mean spin density f pr (&4.3 %) for the tetragonally compressed Cu 2? center in K 2 Zn 1-x Cu x F 4 [29,30]. So, the covalence parameters used seem to be reasonable.…”
Section: Discussionmentioning
confidence: 80%
“…The calculated values are in good agreement with the observed values, suggesting that the parameters (including those related to crystal-field parameters) used in above calculations are suitable. The spin density f pr can be calculated from the observed fluorine hyperfine constants [29,30], and it is related to the covalence parameters (or MO coefficients) N e and k e by the formula: f pr = 1/3 N e (k e ) 2 [31]. The spin density f pr for rhombic Cu 2?…”
Section: Discussionmentioning
confidence: 99%
“…This crystal is used as host for the studies of interaction between 3d n impurity and host lattice. For example, Ba 2 ZnF 6 is one of the few host crystals in which Cu 2+ can be stabilizedby substitution of Zn 2+ -with a d 2 z ground state [2]. So, various spectroscopic studies were made for Ba 2 ZnF 6 doped with 3d n ions [2 -6].…”
Section: Introductionmentioning
confidence: 99%