Abstract
A simple model of alloy nonrandomness is introduced within a framework where the effective concentration of spin singlets as a function of the nominal concentration of magnetic ions in a nonrandom alloy can be obtained by transformations of the corresponding function in random alloys. The theory shows that a given system that is appreciably nonrandom can have a magnetic response almost identical with that of a random distribution. Possible ways of identifying alloy nonrandomness in diluted magnetic semiconductor structures are described.
| Original language | English |
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| Pages (from-to) | 1684-1688 |
| Number of pages | 5 |
| Journal | Journal of Applied Physics |
| Volume | 79 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 1 Feb 1996 |
| Externally published | Yes |