抄録
The electronic structure of bcc ferromagnetic Fe1−xNix, Fe1−xCox, Fe1−xMnx and Fe1−xCrx is discussed on the basis of the coherent potential approximation. The differences in the concentration dependences of the saturation magnetization and the electronic specific heat between Fe1−xNix and Fe1−xCox can be explained reasonably. The calculation yields a good agreement with experiment for Fe1−xMnx and Fe1−xCrx.