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For α=β and g=0 each energy level is twofold degenerate with respect to the s parity. The degenerate states corresponding to even and odd s parities have the same charge densities, and the spin-up and spin-down densities are exchanged.
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For α = β and g = 0 each energy level is twofold degenerate with respect to the s parity. The degenerate states corresponding to even and odd s parities have the same charge densities, and the spin-up and spin-down densities are exchanged.
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Figure presents the case of pure Rashba coupling and g=0. For the pure Dresselhaus coupling the energy spectrum is identical, the average z component of the spin and the s parity are inverted.
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Figure presents the case of pure Rashba coupling and g = 0. For the pure Dresselhaus coupling the energy spectrum is identical, the average z component of the spin and the s parity are inverted.
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