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  • PhysRevB 79 195413

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Disorder-induced pseudodiffusive transport in graphene nanoribbons.

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Disorder-induced pseudodiffusive transport in graphene nanoribbons. / Dietl, P.; Metalidis, G.; Golubev, D. et al.
In: Physical review B, Vol. 79, No. 19, 13.05.2009, p. 195413.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Dietl, P, Metalidis, G, Golubev, D, San-Jose, P, Prada, E, Schomerus, H & Schoen, G 2009, 'Disorder-induced pseudodiffusive transport in graphene nanoribbons.', Physical review B, vol. 79, no. 19, pp. 195413. https://doi.org/10.1103/PhysRevB.79.195413

APA

Dietl, P., Metalidis, G., Golubev, D., San-Jose, P., Prada, E., Schomerus, H., & Schoen, G. (2009). Disorder-induced pseudodiffusive transport in graphene nanoribbons. Physical review B, 79(19), 195413. https://doi.org/10.1103/PhysRevB.79.195413

Vancouver

Dietl P, Metalidis G, Golubev D, San-Jose P, Prada E, Schomerus H et al. Disorder-induced pseudodiffusive transport in graphene nanoribbons. Physical review B. 2009 May 13;79(19):195413. doi: 10.1103/PhysRevB.79.195413

Author

Dietl, P. ; Metalidis, G. ; Golubev, D. et al. / Disorder-induced pseudodiffusive transport in graphene nanoribbons. In: Physical review B. 2009 ; Vol. 79, No. 19. pp. 195413.

Bibtex

@article{a5298f9391304330acab902eb7894447,
title = "Disorder-induced pseudodiffusive transport in graphene nanoribbons.",
abstract = "We study the transition from ballistic to diffusive and localized transport in graphene nanoribbons in the presence of binary disorder, which can be generated by chemical adsorbates or substitutional doping. We show that the interplay between the induced average doping (arising from the nonzero average of the disorder) and impurity scattering modifies the traditional picture of phase-coherent transport. Close to the Dirac point, intrinsic evanescent modes produced by the impurities dominate transport at short lengths giving rise to a regime analogous to pseudodiffusive transport in clean graphene, but without the requirement of heavily doped contacts. This intrinsic pseudodiffusive regime precedes the traditional ballistic, diffusive, and localized regimes. The last two regimes exhibit a strongly modified effective number of propagating modes and a mean free path which becomes anomalously large close to the Dirac point.",
author = "P. Dietl and G. Metalidis and D. Golubev and P. San-Jose and E. Prada and Henning Schomerus and G. Schoen",
note = "{\textcopyright} 2009 The American Physical Society",
year = "2009",
month = may,
day = "13",
doi = "10.1103/PhysRevB.79.195413",
language = "English",
volume = "79",
pages = "195413",
journal = "Physical review B",
issn = "1550-235X",
publisher = "AMER PHYSICAL SOC",
number = "19",

}

RIS

TY - JOUR

T1 - Disorder-induced pseudodiffusive transport in graphene nanoribbons.

AU - Dietl, P.

AU - Metalidis, G.

AU - Golubev, D.

AU - San-Jose, P.

AU - Prada, E.

AU - Schomerus, Henning

AU - Schoen, G.

N1 - © 2009 The American Physical Society

PY - 2009/5/13

Y1 - 2009/5/13

N2 - We study the transition from ballistic to diffusive and localized transport in graphene nanoribbons in the presence of binary disorder, which can be generated by chemical adsorbates or substitutional doping. We show that the interplay between the induced average doping (arising from the nonzero average of the disorder) and impurity scattering modifies the traditional picture of phase-coherent transport. Close to the Dirac point, intrinsic evanescent modes produced by the impurities dominate transport at short lengths giving rise to a regime analogous to pseudodiffusive transport in clean graphene, but without the requirement of heavily doped contacts. This intrinsic pseudodiffusive regime precedes the traditional ballistic, diffusive, and localized regimes. The last two regimes exhibit a strongly modified effective number of propagating modes and a mean free path which becomes anomalously large close to the Dirac point.

AB - We study the transition from ballistic to diffusive and localized transport in graphene nanoribbons in the presence of binary disorder, which can be generated by chemical adsorbates or substitutional doping. We show that the interplay between the induced average doping (arising from the nonzero average of the disorder) and impurity scattering modifies the traditional picture of phase-coherent transport. Close to the Dirac point, intrinsic evanescent modes produced by the impurities dominate transport at short lengths giving rise to a regime analogous to pseudodiffusive transport in clean graphene, but without the requirement of heavily doped contacts. This intrinsic pseudodiffusive regime precedes the traditional ballistic, diffusive, and localized regimes. The last two regimes exhibit a strongly modified effective number of propagating modes and a mean free path which becomes anomalously large close to the Dirac point.

U2 - 10.1103/PhysRevB.79.195413

DO - 10.1103/PhysRevB.79.195413

M3 - Journal article

VL - 79

SP - 195413

JO - Physical review B

JF - Physical review B

SN - 1550-235X

IS - 19

ER -