We present a theory of magnetic anisotropy in III1−xMnxV diluted magnetic semiconductors with carrier-induced
ferromagnetism. The theory is based on four and six band envelope functions
models for the valence band holes and a mean-field treatment of their exchange
interactions with Mn++ ions. We find that easy-axis reorientations
can occur as a function of temperature, carrier density p, and strain. The
magnetic anisotropy in strain-free samples is predicted to have a p5/3
hole-density dependence at small p, a p−1 dependence at large p, and
remarkably large values at intermediate densities. An explicit expression,
valid at small p, is given for the uniaxial contribution to the magnetic
anisotropy due to unrelaxed epitaxial growth lattice-matching strains. Results
of our numerical simulations are in agreement with magnetic anisotropy
measurements on samples with both compressive and tensile strains. We predict
that decreasing the hole density in current samples will lower the
ferromagnetic transition temperature, but will increase the magnetic anisotropy
energy and the coercivity.Comment: 15 pages, 15 figure