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Volumn 82, Issue 11, 2010, Pages

Topological defects and gapless modes in insulators and superconductors

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EID: 77957709555     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.82.115120     Document Type: Article
Times cited : (1004)

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    • -2. One could mathematically remove the bulk topological obstruction by adding a defectless Hamiltonian H (k,r ) =H (k,r ) H0 (k).
    • -2. One could mathematically remove the bulk topological obstruction by adding a defectless Hamiltonian H (k,r ) =H (k,r ) H0 (k).
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    • Again, assume the bulk has trivial topology. Or otherwise remove the topological obstruction mathematically by adding a defectless Hamiltonian.
    • Again, assume the bulk has trivial topology. Or otherwise remove the topological obstruction mathematically by adding a defectless Hamiltonian.
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    • Deformation of Hamiltonians on ∂ T1/2 (s), for s∈ [0,1 ] has dimension δ= (d-1 ) - (d-1+1+1 ) =-2, and is classified by 2Z.
    • Deformation of Hamiltonians on ∂ T 1 / 2 (s), for s ∈ [0, 1] has dimension δ = (d - 1) - (d - 1 + 1 + 1) = - 2, and is classified by 2 Z.


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