Abstract
An infinite-order perturbation approach to the theory of magnetism in magnets with strong single-ion anisotropy is given. This approach is based on a canonical transformation of the system into one with a diagonal crystal field, an effective two-ion anisotropy, and reduced ground-state corrections. A matrix-element matching procedure is used to obtain an explicit expression for the spin-wave energy to second order. The consequences of this theory are illustrated by an application to a simple example with planar anisotropy and an external magnetic field. A detailed comparison between the results of this and the conventional approach is discussed.
© 1977 The American Physical Society
| Original language | English |
|---|---|
| Journal | Physical Review B |
| Volume | 16 |
| Issue number | 1 |
| Pages (from-to) | 408-418 |
| ISSN | 2469-9950 |
| DOIs | |
| Publication status | Published - 1977 |