Abstract
The phase diagram of a quenched random alloy of two components with competing anisotropies exhibits two critical lines, corresponding to ordering of only m1 (or m2) spin components. The two lines meet at a tetracritical point, where all m=m1+m2 components order simultaneously. General scaling arguments are used to show that the critical behavior at this point is decoupled, i.e., the m1- and m2-component subsystems have separate scaling free energies. Applications and experiments are briefly discussed.
| Original language | English |
|---|---|
| Pages (from-to) | 1587-1590 |
| Number of pages | 4 |
| Journal | Physical Review Letters |
| Volume | 37 |
| Issue number | 23 |
| DOIs | |
| State | Published - 1976 |
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