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The two Bloch walls shown in Fig. 2 are energetically degenerate if the crystal structure possesses a mirror plane parallel to the propagation direction. In order to see this, note that the spin-orbit Hamiltonian in the absence of an external magnetic field commutes with a symmetry operation that simultaneously transforms (rx, ry, rz) → (rx, - ry, rz) in real space and (Mx, My, Mz) → (Mx, - My, Mz) in spin space.
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The two Bloch walls shown in Fig. 2 are energetically degenerate if the crystal structure possesses a mirror plane parallel to the propagation direction. In order to see this, note that the spin-orbit Hamiltonian in the absence of an external magnetic field commutes with a symmetry operation that simultaneously transforms (rx, ry, rz) → (rx, - ry, rz) in real space and (Mx, My, Mz) → (Mx, - My, Mz) in spin space
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For program description see
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For program description see http://www.flapw.de
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The even part of the SOC-induced corrections to E (λ-1) is negligible compared to the scalar-relativistic values given in Fig. 4.
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The even part of the SOC-induced corrections to E (λ-1) is negligible compared to the scalar-relativistic values given in Fig. 4
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