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Discrepancies in the nature of the CaRuO3 magnetic ground state exist in the theoretical literature, with the findings often depending on the method used. For example, early density-functional theory calculations predicted that CaRuO3 is ferromagnetic (Ref.); more recent results reported a G -type antiferromagnetic ground state (Ref.). Separate studies also indicated that CaRuO3 can be ferromagnetic but that the ferromagnetic ground state is metastable with respect to the most stable nonmagnetic solution (Ref.). In our calculations, the fully relaxed ground-state structure is nonmagnetic.
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Discrepancies in the nature of the CaRuO3 magnetic ground state exist in the theoretical literature, with the findings often depending on the method used. For example, early density-functional theory calculations predicted that CaRuO3 is ferromagnetic (Ref.); more recent results reported a G -type antiferromagnetic ground state (Ref.). Separate studies also indicated that CaRuO3 can be ferromagnetic but that the ferromagnetic ground state is metastable with respect to the most stable nonmagnetic solution (Ref.). In our calculations, the fully relaxed ground-state structure is nonmagnetic.
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In our first-principles calculations, a nonmagnetic ground state is understood as one in which there is an absence of spin polarization. An ab initio simulation of a paramagnetic state is beyond the scope of this work. In the remainder of the paper, we remember that although CaRuO3 is paramagnetic experimentally, we only consider in our calculations nonmagnetic, ferromagnetic, and antiferromagnetic solutions.
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In our first-principles calculations, a nonmagnetic ground state is understood as one in which there is an absence of spin polarization. An ab initio simulation of a paramagnetic state is beyond the scope of this work. In the remainder of the paper, we remember that although CaRuO3 is paramagnetic experimentally, we only consider in our calculations nonmagnetic, ferromagnetic, and antiferromagnetic solutions.
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