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We present a comprehensive theory of the temperature- and disorder-dependence of half-metallic ferrimagnetism in the double perovskite SrFeMoO (SFMO) with above room temperature. We show that the magnetization and conduction electron polarization are both proportional to the magnetization of localized Fe spins. We derive and validate an effective spin Hamiltonian, amenable to large-scale three-dimensional simulations. We show how and are affected by disorder, ubiquitous in these materials. We suggest a way to enhance in SFMO without sacrificing polarization.

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