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The electronic configurations for each atom is Sr4 s2 4 p6 4 d0 4 f0 (1.50, 1.50, 2.00, 2.00), Ru4 s2 4 p6 4 d7 4 f0 (1.30, 1.30, 1.40, 1.30), and O2 s2 2 p4 3 d0 4 f0 (1.15, 1.15, 1.15, 1.50), where the cutoff radii for each orbital is given in parentheses.
-
The electronic configurations for each atom is Sr4 s2 4 p6 4 d0 4 f0 (1.50, 1.50, 2.00, 2.00), Ru4 s2 4 p6 4 d7 4 f0 (1.30, 1.30, 1.40, 1.30), and O2 s2 2 p4 3 d0 4 f0 (1.15, 1.15, 1.15, 1.50), where the cutoff radii for each orbital is given in parentheses.
-
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50
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54449096249
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The grid cutoff mentioned is not directly comparable to the plane-wave cutoff value used to represent the wave functions in a standard plane-wave implementation of DFT; it is rather used here to represent the density, and is typically four times larger than the wave function cutoff.
-
The grid cutoff mentioned is not directly comparable to the plane-wave cutoff value used to represent the wave functions in a standard plane-wave implementation of DFT; it is rather used here to represent the density, and is typically four times larger than the wave function cutoff.
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Although in this symmetry the RuO6 cages are rotated, we retain the standard spherical harmonics for the 4d orbitals described in terms of an octahedral crystal field for a cubic perovskite. The transformation from the cubic to orthorhombic d orbital reference frame requires a rotation of π/4 about the [001] direction; additionally, the octahedral units retain almost all of their integrity; i.e., the apical and axial Ru-O bond lengths are identical within 0.01 Å.
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Although in this symmetry the RuO6 cages are rotated, we retain the standard spherical harmonics for the 4d orbitals described in terms of an octahedral crystal field for a cubic perovskite. The transformation from the cubic to orthorhombic d orbital reference frame requires a rotation of π/4 about the [001] direction; additionally, the octahedral units retain almost all of their integrity; i.e., the apical and axial Ru-O bond lengths are identical within 0.01 Å.
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The material preparation and characterization follows that outlined in PRBMDO 0163-1829 10.1103/PhysRevB.60.2281
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Complete structural relaxation of the three-unit-cell slab within the orthorhombic symmetry did not produce significant changes in the electronic or magnetic structure.
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Complete structural relaxation of the three-unit-cell slab within the orthorhombic symmetry did not produce significant changes in the electronic or magnetic structure.
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