2008
DOI: 10.1103/physrevlett.100.177207
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Spin Currents in Rough Graphene Nanoribbons: Universal Fluctuations and Spin Injection

Abstract: We investigate spin conductance in zigzag graphene nanoribbons and propose a spin injection mechanism based only on graphitic nanostructures. We find that nanoribbons with atomically straight, symmetric edges show zero spin conductance but nonzero spin Hall conductance. Only nanoribbons with asymmetrically shaped edges give rise to a finite spin conductance and can be used for spin injection into graphene. Furthermore, nanoribbons with rough edges exhibit mesoscopic spin conductance fluctuations with a univers… Show more

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Cited by 304 publications
(194 citation statements)
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“…Second, the fact that our treatment of the zigzag-edge-associated average level density proves adequate for both settings, models without and with particle-hole breaking effects, e.g., from next-nearestneighbor coupling (see Sec. III C 2, encourages us to address zigzag edge magnetism 19,[74][75][76] within this framework. Third, the semiclassical formalism developed allows for treating graphene nanostructures with boundaries that can be viewed as being composed of many zigzag-and armchair-edge segments.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Second, the fact that our treatment of the zigzag-edge-associated average level density proves adequate for both settings, models without and with particle-hole breaking effects, e.g., from next-nearestneighbor coupling (see Sec. III C 2, encourages us to address zigzag edge magnetism 19,[74][75][76] within this framework. Third, the semiclassical formalism developed allows for treating graphene nanostructures with boundaries that can be viewed as being composed of many zigzag-and armchair-edge segments.…”
Section: Discussionmentioning
confidence: 99%
“…Similar edge potentials can model also adsorbents at graphene edges or edge magnetism. 29,76 The Dirac equation together with the Bloch theorem gives, for the y-dependent part of the wave functions in the valley τ = +1, Now we integrate these equations over a small window [y 0 − ε,y 0 + ε] around the potential and take the limit ε → 0 afterward. Assuming that ψ has at most a finite discontinuity at y 0 , we obtain from Eq.…”
Section: Discussionmentioning
confidence: 99%
“…Several experimental studies provide direct [10,[14][15][16] or indirect [17] evidence for the presence of the edge states also in supported GNRs, albeit without probing its magnetism. Such edge states might be exploited for a multitude of spintronics applications [4,[18][19][20], but so far it is unclear, if the edge states contribute to the measured transport properties of nanostructures at all [21]. Thus, it is important to elucidate the role of the substrate and of edge termination.…”
Section: Pacs Numbersmentioning
confidence: 99%
“…Graphene nanoribbons are quasi-one-dimensional structures with electronic properties depending on the angle at which they are cut. This includes a tunable energy gap with semimetallic or semiconductor behavior, [13][14][15] one-dimensional edge states at the Fermi level with unusual magnetic properties with possible spintronic applications, [16][17][18][19][20][21][22][23] and solitonic edge states as in polyacetylene. [37][38][39] Graphene nanoribbons also played an important role in inspiring the field of topological insulators.…”
Section: Introductionmentioning
confidence: 99%