Abstract
The scaling equation of state for ferromagnets with interactions of cubic symmetry is derived to first order in ε=4-d, where d is the dimensionality of space. Finite susceptibilities are found at zero field below Tc. These diverge, however, as the number of spin components approaches nc (3.13 at ε=1) from above, where the cubic fixed point coincides with the usual Heisenberg fixed point.
Original language | English |
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Pages (from-to) | 3006-3009 |
Number of pages | 4 |
Journal | Physical Review B |
Volume | 10 |
Issue number | 7 |
DOIs | |
State | Published - 1 Jan 1974 |
Externally published | Yes |
ASJC Scopus subject areas
- Condensed Matter Physics