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Diamagnetic effects are included in the calculation of the electrical resistivity of a Bloch wall in a ferromagnetic metal. The resulting electron orbits, which are convoluted zig‐zag‐ging trajectories near the wall, produce an increase in the resistivity which is roughly proportional to (ω c τ) 2 , where ω c is the cyclotron frequency of the electron due to the internal magnetization. Such an effect explains satisfactorily the experimental data reported in the literature.
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Cabrera et al. (1974) studied this question.
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