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Volumn 79, Issue 19, 2009, Pages

Topological phases and the quantum spin Hall effect in three dimensions

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EID: 67649407761     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.195322     Document Type: Article
Times cited : (1064)

References (24)
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    • As stated previously, the associated Hamiltonian need not be the Hamiltonian of the system but one which has the same ground state.
    • As stated previously, the associated Hamiltonian need not be the Hamiltonian of the system but one which has the same ground state.
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    • We refer to continuous wave functions of this sort as bands which do not touch in momentum space.
    • We refer to continuous wave functions of this sort as bands which do not touch in momentum space.
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    • We can always choose the paths such that the diabolical points do not map onto themselves under time reversal.
    • We can always choose the paths such that the diabolical points do not map onto themselves under time reversal.
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    • This follows from the definition of the Z2 invariant in Eq. 8.
    • This follows from the definition of the Z2 invariant in Eq. 8.
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    • An analysis through K theory seems to suggest that the fourth Z2 invariant or the monopole charge described above arises from the twisted KR theory of S3 while the remaining three arise from the faces of T3 (Ref.).
    • An analysis through K theory seems to suggest that the fourth Z2 invariant or the monopole charge described above arises from the twisted KR theory of S3 while the remaining three arise from the faces of T3 (Ref.).
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