Abstract
We investigate whether the electric field dradient (EFG) at an atomic site in the unit cell of a periodic solid can be modeled via the electrostatic field gradient set up by atomic point charges outside that site. To test this approach we contrast the EFG predicted by such point-ion models for long-range ordered GaIn P2 alloys with the results obtained from self-consistent all-electroncalculations in the local density approximation (LDA). We first tested our LDA approach for ZnAl2O4, for which experimental data exist, , finding the quadrupole coupling constant Qcc(27AL)=3.94 MHz, compared with the measured value of |Q|=3.69 MHz. Applying next the LDA approach to perfectly ordered GaInP2 (for which experimental data do not exist), we find the LDA quadrupole coupling constantQcc+4.83, -2.84 and 13.08 MHz for 69Ga, 71Ga, and 115In, respectively. We further find that more than 95% of these EFGs originate from the anistropic electron charge distribution within a small sphere of radius more or less 0.2 Angstrom about the respective atomic site. Hence, the point-ion model significantly underestimates the magnitude of the EFG (and in some cases also gives an incorrectsign). The point-ion model also fails in reproducing the relative trends in the EFG as the crystal structure changes. We conclude that the point-ion model is not a viable alternative to calculate EFG in periodic covalent solids.
Original language | American English |
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Pages (from-to) | 1931-1935 |
Number of pages | 5 |
Journal | The Journal of Chemical Physics |
Volume | 107 |
Issue number | 6 |
DOIs | |
State | Published - 1997 |
NREL Publication Number
- NREL/JA-590-22093