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Volumn 84, Issue 15, 2011, Pages

Zigzag graphene nanoribbon edge reconstruction with Stone-Wales defects

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Indexed keywords


EID: 80455156032     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.84.155435     Document Type: Article
Times cited : (77)

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    • The numerical diagonalization of the tight-binding Hamiltonian was performed using the tools of the lapack numerical library
    • The numerical diagonalization of the tight-binding Hamiltonian was performed using the tools of the lapack numerical library.
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    • -(k)=0 requires det[M(k)]=0; we found no relevant limits where this is verified.
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    • 4=0, though we do not present the corresponding data.
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    • The whole spectrum is shifted in ka, because we have set n=0 at the upper edge (where n is the label of the zigzag rows). If we set n=0 to the center of the ribbon, the shift would disappear (Ref. 24)
    • The whole spectrum is shifted in ka, because we have set n=0 at the upper edge (where n is the label of the zigzag rows). If we set n=0 to the center of the ribbon, the shift would disappear (Ref. 24).


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