Abstract
We develop a theory for the spin waves in a dilute Heisenberg ferromagnet. The d-dimensional bond percolating network of ferromagnetic spins is solved within the effective-medium approximation. It is shown that these excitations obey a classical equation of motion. We have found that for 2<d<4, there is a critical frequency ωc, consistent with the mobility edge, such that ωc scales as (ppc)2. When ω<ωc, the excitations are extended, while when ω>ωc, they are localized. We also found that there is a rapid increase in the density of states at the mobility edge. The jump near the mobility edge is found to scale as (ppc)1(d2).

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