The wave-vector (q) and doping $(x,y)$ dependences of the magnetic energy, iron moment, and effective exchange interactions in LaFeAsO_1-xFₓ and Ba_1-2yK2yFe₂As₂ are studied by self-consistent LSDA calculations for co-planar spin spirals. For the undoped compounds $(x=0,y=0)$, the minimum of the calculated total energy, E(q), is for q corresponding to stripe antiferromagnetic order. Already at low levels of electron doping $(x)$, this minimum becomes flat in LaFeAsO_1-xFₓ and for x5%, it shifts to an incommensurate q. In Ba_1-2yK2yFe₂As₂, stripe order remains stable for hole doping up to $y=0.3$. These results are explained in terms of the band structure. The magnetic interactions cannot be accurately described by a simple classical Heisenberg model and the effective exchange interactions fitted to E(q) depend strongly on doping. The doping dependence of the E(q) curves is compared with that of the noninteracting magnetic susceptibility for which similar trends are found.
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Yaresko et al. (2009) studied this question.
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