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Electron density distribution and screening in rippled graphene sheets

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Electron density distribution and screening in rippled graphene sheets. / Gibertini, Marco; Tomadin, Andrea; Polini, Marco et al.
In: Physical review B, Vol. 81, 125437, 15.03.2010.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Gibertini, M, Tomadin, A, Polini, M, Fasolino, A & Katsnelson, MI 2010, 'Electron density distribution and screening in rippled graphene sheets', Physical review B, vol. 81, 125437. https://doi.org/10.1103/PhysRevB.81.125437

APA

Gibertini, M., Tomadin, A., Polini, M., Fasolino, A., & Katsnelson, M. I. (2010). Electron density distribution and screening in rippled graphene sheets. Physical review B, 81, Article 125437. https://doi.org/10.1103/PhysRevB.81.125437

Vancouver

Gibertini M, Tomadin A, Polini M, Fasolino A, Katsnelson MI. Electron density distribution and screening in rippled graphene sheets. Physical review B. 2010 Mar 15;81:125437. doi: 10.1103/PhysRevB.81.125437

Author

Gibertini, Marco ; Tomadin, Andrea ; Polini, Marco et al. / Electron density distribution and screening in rippled graphene sheets. In: Physical review B. 2010 ; Vol. 81.

Bibtex

@article{05b30bdfdf7d44c7a473ca08a674d116,
title = "Electron density distribution and screening in rippled graphene sheets",
abstract = "Single-layer graphene sheets are typically characterized by long-wavelength corrugations (ripples) which can be shown to be at the origin of rather strong potentials with both scalar and vector components. We present an extensive microscopic study, based on a self-consistent Kohn-Sham-Dirac density-functional method, of the carrier-density distribution in the presence of these ripple-induced external fields. We find that spatial density fluctuations are essentially controlled by the scalar component, especially in nearly neutral graphene sheets, and that in-plane atomic displacements are as important as out-of-plane ones. The latter fact is at the origin of a complicated spatial distribution of electron-hole puddles which has no evident correlation with the out-of-plane topographic corrugations. In the range of parameters we have explored, exchange and correlation contributions to the Kohn-Sham potential seem to play a minor role.",
author = "Marco Gibertini and Andrea Tomadin and Marco Polini and A. Fasolino and Katsnelson, {M. I.}",
year = "2010",
month = mar,
day = "15",
doi = "10.1103/PhysRevB.81.125437",
language = "English",
volume = "81",
journal = "Physical review B",
issn = "1098-0121",
publisher = "AMER PHYSICAL SOC",

}

RIS

TY - JOUR

T1 - Electron density distribution and screening in rippled graphene sheets

AU - Gibertini, Marco

AU - Tomadin, Andrea

AU - Polini, Marco

AU - Fasolino, A.

AU - Katsnelson, M. I.

PY - 2010/3/15

Y1 - 2010/3/15

N2 - Single-layer graphene sheets are typically characterized by long-wavelength corrugations (ripples) which can be shown to be at the origin of rather strong potentials with both scalar and vector components. We present an extensive microscopic study, based on a self-consistent Kohn-Sham-Dirac density-functional method, of the carrier-density distribution in the presence of these ripple-induced external fields. We find that spatial density fluctuations are essentially controlled by the scalar component, especially in nearly neutral graphene sheets, and that in-plane atomic displacements are as important as out-of-plane ones. The latter fact is at the origin of a complicated spatial distribution of electron-hole puddles which has no evident correlation with the out-of-plane topographic corrugations. In the range of parameters we have explored, exchange and correlation contributions to the Kohn-Sham potential seem to play a minor role.

AB - Single-layer graphene sheets are typically characterized by long-wavelength corrugations (ripples) which can be shown to be at the origin of rather strong potentials with both scalar and vector components. We present an extensive microscopic study, based on a self-consistent Kohn-Sham-Dirac density-functional method, of the carrier-density distribution in the presence of these ripple-induced external fields. We find that spatial density fluctuations are essentially controlled by the scalar component, especially in nearly neutral graphene sheets, and that in-plane atomic displacements are as important as out-of-plane ones. The latter fact is at the origin of a complicated spatial distribution of electron-hole puddles which has no evident correlation with the out-of-plane topographic corrugations. In the range of parameters we have explored, exchange and correlation contributions to the Kohn-Sham potential seem to play a minor role.

U2 - 10.1103/PhysRevB.81.125437

DO - 10.1103/PhysRevB.81.125437

M3 - Journal article

VL - 81

JO - Physical review B

JF - Physical review B

SN - 1098-0121

M1 - 125437

ER -