Abstract
The relativistic contribution to the quadrupolar hyperfine interaction in systems with nonvanishing orbital moment is treated in terms of a nonrelativistic description of the wave function in these systems. The Sandars-Beck theory, originally treating S-state ions only, is extended to treat non-S systems. The results are utilized to derive the relativistic quadrupolar contribution in two realistic situations; (a) ionic systems with an orbital singlet ground state, and (b) metallic systems amenable to orthogonal-plane-waves-interpolation-scheme band-structure calculation.
| Original language | English |
|---|---|
| Pages (from-to) | 355-362 |
| Number of pages | 8 |
| Journal | Physical Review B |
| Volume | 17 |
| Issue number | 1 |
| DOIs | |
| State | Published - 1978 |
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