2007
DOI: 10.1103/physrevb.76.155118
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Calibration of the isomer shift for the14.4keVtransition inFe57using the full-potential linearized augmented plane-wave method

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Cited by 81 publications
(60 citation statements)
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“…The numeric value of˛(and of R/R) shows strong dependence on the choice of the particular density functional and the basis set employed in the calculations and can vary by as much as 20-30%. Thus, the values in the range −0.253 to −0.367a 3 0 mm s −1 were obtained by different authors for the calibration constant˛of 57 Fe, which leads to the values of R/R varying in the range −0.89 × 10 −3 to −1.30 × 10 −3 [56,77,81,82]. It should be noticed however that modern density functionals do not correctly describe the electron-electron interaction potential in the vicinity of nucleus.…”
Section: Fe Isomer Shiftmentioning
confidence: 84%
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“…The numeric value of˛(and of R/R) shows strong dependence on the choice of the particular density functional and the basis set employed in the calculations and can vary by as much as 20-30%. Thus, the values in the range −0.253 to −0.367a 3 0 mm s −1 were obtained by different authors for the calibration constant˛of 57 Fe, which leads to the values of R/R varying in the range −0.89 × 10 −3 to −1.30 × 10 −3 [56,77,81,82]. It should be noticed however that modern density functionals do not correctly describe the electron-electron interaction potential in the vicinity of nucleus.…”
Section: Fe Isomer Shiftmentioning
confidence: 84%
“…(7). In these calculations [52][53][54][55][56], the relativistic electron density (obtained in scalar-relativistic formalism with point-charge nucleus) was averaged over a spherical volume with the nuclear charge radius (3). In atomic calculations, a similar approach was used by Mallow et al [50] to bypass a singularity of the relativistic wave function obtained with the point-charge nucleus.…”
Section: Relativistic Effectsmentioning
confidence: 99%
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