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In itinerant electron ferromagnets, spectral weight is transferred at finite temperatures from quasiparticle peaks located at majority- and minority-spin band energies to shadow-band peaks. For a given Bloch wave vector and band index, the majority-spin shadow-band peak is located near the minority-spin quasiparticle energy and the minority-spin shadow-band peak is located near the majority-spin quasiparticle energy. This property can explain much of the temperature dependence seen in the magnetoresistance of magnetic tunnel junctions.
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MacDonald et al. (1998) studied this question.
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