2018
DOI: 10.1103/physrevb.98.045419
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Braiding of edge states in narrow zigzag graphene nanoribbons: Effects of third-neighbor hopping on transport and magnetic properties

Abstract: We study narrow zigzag graphene nanoribbons (ZGNRs), employing density functional theory (DFT) simulations and the tight-binding (TB) method. The main result of these calculations is the braiding of the conduction and valence bands, generating Dirac cones for non-commensurate wave vectors k. Employing a TB Hamiltonian, we show that the braiding is generated by the thirdneighbor hopping (N3). We calculate the band structure, the density of states and the conductance, new conductance channels are opened, and the… Show more

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Cited by 10 publications
(7 citation statements)
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“…This could explain the previous LDA outcome published in Ref. 4, which reports an AFM stabilization energy of a few meV, while in our case the AFM gain is null. The sensitiveness to k-points sampling is clearly due to a Dirac cone formation in the PM band structure, arising from edge states 4 .…”
Section: B Ground-state Properties From Dft and Comparison With Qmcsupporting
confidence: 76%
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“…This could explain the previous LDA outcome published in Ref. 4, which reports an AFM stabilization energy of a few meV, while in our case the AFM gain is null. The sensitiveness to k-points sampling is clearly due to a Dirac cone formation in the PM band structure, arising from edge states 4 .…”
Section: B Ground-state Properties From Dft and Comparison With Qmcsupporting
confidence: 76%
“…4, which reports an AFM stabilization energy of a few meV, while in our case the AFM gain is null. The sensitiveness to k-points sampling is clearly due to a Dirac cone formation in the PM band structure, arising from edge states 4 . This is particulary evident in the 2-ZGNR, while the Dirac velocities flatten out for larger n-ZGNR, yielding a braided band structure.…”
Section: B Ground-state Properties From Dft and Comparison With Qmccontrasting
confidence: 41%
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“…1(D), the 3-ZGNR exhibits valence and conduction band braiding with two degenerate Dirac-points; a commensurate one at the BZ boundary and other incommensurate degeneracy at k k $ 1.1 A À1 , in agreement with DFT and third NN-TB calculations. 29 This metallic band structure is preserved for chevron polymer of higher N, but with a single commensurate degeneracy at BZ boundary. The effect of different N values only shows up as relatively atter dispersion (i.e., smaller Fermi velocity v F ) for polymers with longer arms, yet the degeneracy point is unaltered.…”
Section: Methodsmentioning
confidence: 87%
“…These two shortcomings can both be avoided by invoking the narrowest zigzag graphene nanoribbon (nZGNR) which is made up of linearly fused benzene rings. First, zigzag graphene nanoribbons (ZGNRs) possess nonzero bandgaps tuned by the width, with the nZGNR showing the largest bandgap. Second, the nZGNR has spin-polarized electronic states along the two edges, , as widely studied for broader ZGNRs. , These quasi-one-dimensional systems have higher spin wave stiffness than traditional magnetic materials and thus possess relatively long spin correlation lengths . Given that the coupling strength between the spins along the two opposite edges increases when the width of the ZGNRs decreases, the nZGNR will have the strongest interedge interactions. , Moreover, the nZGNR has the largest magnetoresistance among the ZGNR family .…”
Section: Introductionmentioning
confidence: 99%