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Electron-doped metallic states of Ca1−xYxVO3 and Ca1−xYxTiO3 change into non-metallic states around x∼0.4 and 0.6, respectively. The residual resistivity in the metallic states increases with increasing effective magnetic moment or coefficient of T2 term of resistivity. The effective moment reaches ∼ 0.5 µB/molecule in Ca1−xYxVO3 and also in Ca1−xYxTiO3 near the metal-nonmetal phase boundary...
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