Abstract
The magnetic phase diagram of γ-Mn alloys contains both collinear and noncollinear magnetic phases in fct and fcc crystal structures. Using a two-band model which incorporates the magnetoelastic coupling, we find that the gap in the spin-wave dispersion is proportional to the 3/2 power of the sublattice magnetization in agreement with experiments on both the collinear and noncollinear magnetic phases. For the noncollinear magnetic phases observed in MnNi and FeMn alloys, high-frequency excitations are predicted with where 2Δ is the energy gap in the quasiparticle spectrum.
- Received 13 February 1998
DOI:https://doi.org/10.1103/PhysRevB.58.R5912
©1998 American Physical Society