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Volumn 80, Issue 19, 2009, Pages

Spin-orbit coupling effects in two-dimensional circular quantum rings: Elliptical deformation of confined electron density

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EID: 77954702272     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.195319     Document Type: Article
Times cited : (45)

References (57)
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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.
    • 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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    • The eigenstates of σx - σy can be constructed from the odd and the even s-parity eigenstates which in the case of α=β and g=0 correspond to degenerate energy levels. The eigenstates of σx - σy are no longer s -parity eigenstates.
    • The eigenstates of σ x - σ y can be constructed from the odd and the even s-parity eigenstates which in the case of α = β and g = 0 correspond to degenerate energy levels. The eigenstates of σ x - σ y are no longer s -parity eigenstates.
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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.
    • 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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