One-dimensional electron systems on graphene edges

In this dissertation several aspects on one-dimensional edge states in grapheme are studied. First, a background in the history and development of graphitic forms is presented. Then some novel features found in two-dimensional bulk graphene are presented. Here, some focus is given to the chiral natu...

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Main Author: Hill, Jason Edward, 1978-
Other Authors: MacDonald, Allan H.
Format: Others
Language:English
Published: 2008
Subjects:
Online Access:http://hdl.handle.net/2152/3797
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spelling ndltd-UTEXAS-oai-repositories.lib.utexas.edu-2152-37972015-09-20T16:52:44ZOne-dimensional electron systems on graphene edgesHill, Jason Edward, 1978-GraphiteNanostructured materialsNuclear spinIn this dissertation several aspects on one-dimensional edge states in grapheme are studied. First, a background in the history and development of graphitic forms is presented. Then some novel features found in two-dimensional bulk graphene are presented. Here, some focus is given to the chiral nature of the Dirac equation and the symmetries found in the grahene. Magnetism and interactions in graphene is also briefly discussed. Finally, the graphene nanoribbon with its two typical edges: armchair and zigzag is introduced. Gaps due to finite-size effects are studied. Next, the problem of determining the zigzag ground state is presented. Later, we develop this in an attempt to add the Coulomb interaction to the zigzag flat-band states. These nanoribbons can be stimulated with a tight-binding code on a lattice model in which many different effects can be added, including an A/B sublattice asymmetry, spin-orbit coupling and external fields. The lowest Landau level solutions in the different ribbon orientations is of particular current interest. This is done in the context of understanding new physics and developing novel applications of graphene nanoribbon devices. Adding spin-orbit to a graphene ribbon Hamiltonian leads to current carrying electronic states localized on the sample edges. These states can appear on both zigzag and armchair edges in the semi-finite limit and differ qualitatively in dispersion and spin-polarization from the well known zigzag edge states that occur in models that do not include spin-orbit coupling. We investigate the properties of these states both analytically and numerically using lattice and continuum models with intrinsic and Rashba spin-orbit coupling and spin-independent gap producing terms. A brief discussion of the Berry curvature and topological numbers of graphene with spin-orbit coupling also follows.MacDonald, Allan H.2008-08-29T00:11:07Z2008-08-29T00:11:07Z2007-122008-08-29T00:11:07ZThesiselectronichttp://hdl.handle.net/2152/3797221346809engCopyright © is held by the author. Presentation of this material on the Libraries' web site by University Libraries, The University of Texas at Austin was made possible under a limited license grant from the author who has retained all copyrights in the works.
collection NDLTD
language English
format Others
sources NDLTD
topic Graphite
Nanostructured materials
Nuclear spin
spellingShingle Graphite
Nanostructured materials
Nuclear spin
Hill, Jason Edward, 1978-
One-dimensional electron systems on graphene edges
description In this dissertation several aspects on one-dimensional edge states in grapheme are studied. First, a background in the history and development of graphitic forms is presented. Then some novel features found in two-dimensional bulk graphene are presented. Here, some focus is given to the chiral nature of the Dirac equation and the symmetries found in the grahene. Magnetism and interactions in graphene is also briefly discussed. Finally, the graphene nanoribbon with its two typical edges: armchair and zigzag is introduced. Gaps due to finite-size effects are studied. Next, the problem of determining the zigzag ground state is presented. Later, we develop this in an attempt to add the Coulomb interaction to the zigzag flat-band states. These nanoribbons can be stimulated with a tight-binding code on a lattice model in which many different effects can be added, including an A/B sublattice asymmetry, spin-orbit coupling and external fields. The lowest Landau level solutions in the different ribbon orientations is of particular current interest. This is done in the context of understanding new physics and developing novel applications of graphene nanoribbon devices. Adding spin-orbit to a graphene ribbon Hamiltonian leads to current carrying electronic states localized on the sample edges. These states can appear on both zigzag and armchair edges in the semi-finite limit and differ qualitatively in dispersion and spin-polarization from the well known zigzag edge states that occur in models that do not include spin-orbit coupling. We investigate the properties of these states both analytically and numerically using lattice and continuum models with intrinsic and Rashba spin-orbit coupling and spin-independent gap producing terms. A brief discussion of the Berry curvature and topological numbers of graphene with spin-orbit coupling also follows.
author2 MacDonald, Allan H.
author_facet MacDonald, Allan H.
Hill, Jason Edward, 1978-
author Hill, Jason Edward, 1978-
author_sort Hill, Jason Edward, 1978-
title One-dimensional electron systems on graphene edges
title_short One-dimensional electron systems on graphene edges
title_full One-dimensional electron systems on graphene edges
title_fullStr One-dimensional electron systems on graphene edges
title_full_unstemmed One-dimensional electron systems on graphene edges
title_sort one-dimensional electron systems on graphene edges
publishDate 2008
url http://hdl.handle.net/2152/3797
work_keys_str_mv AT hilljasonedward1978 onedimensionalelectronsystemsongrapheneedges
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