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Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields

One of the most striking properties of graphene is the relativistic-like Dirac-Cone spectrum of charge carriers. By applying high-frequency laser fields, the system can be described with the use of similar spectrum which is based on a concept of electron quasi-energy. There in this spectrum a creati...

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Main Authors: Shahd A.A. Alfadhli, Feodor Kusmartsev, Sergey Saveliev
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Published: 2019
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Online Access:https://hdl.handle.net/2134/37660
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author Shahd A.A. Alfadhli
Feodor Kusmartsev
Sergey Saveliev
author_facet Shahd A.A. Alfadhli
Feodor Kusmartsev
Sergey Saveliev
author_sort Shahd A.A. Alfadhli (7170704)
collection Figshare
description One of the most striking properties of graphene is the relativistic-like Dirac-Cone spectrum of charge carriers. By applying high-frequency laser fields, the system can be described with the use of similar spectrum which is based on a concept of electron quasi-energy. There in this spectrum a creation and annihilation of new Dirac points and cones as well as opening a gap may arise. This allows controlling electron motion without applying DC periodic fields which are effectively described by graphene superlattices. Here we demonstrate that coherent electromagnetic fields applied to graphene can generate new Dirac and Weyl points, induce Lifshitz quantum phase transition for slightly doped graphene and produce an anisotropy of the Dirac cones, which can be even infinite.
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institution Loughborough University
publishDate 2019
record_format Figshare
spelling rr-article-94080352019-04-15T00:00:00Z Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields Shahd A.A. Alfadhli (7170704) Feodor Kusmartsev (1251207) Sergey Saveliev (1250619) Other physical sciences not elsewhere classified Solid state and materials Physical Sciences not elsewhere classified One of the most striking properties of graphene is the relativistic-like Dirac-Cone spectrum of charge carriers. By applying high-frequency laser fields, the system can be described with the use of similar spectrum which is based on a concept of electron quasi-energy. There in this spectrum a creation and annihilation of new Dirac points and cones as well as opening a gap may arise. This allows controlling electron motion without applying DC periodic fields which are effectively described by graphene superlattices. Here we demonstrate that coherent electromagnetic fields applied to graphene can generate new Dirac and Weyl points, induce Lifshitz quantum phase transition for slightly doped graphene and produce an anisotropy of the Dirac cones, which can be even infinite. 2019-04-15T00:00:00Z Text Journal contribution 2134/37660 https://figshare.com/articles/journal_contribution/Manipulating_the_anisotropy_of_the_Dirac-Cone_in_graphene_by_laser_fields/9408035 CC BY 4.0
spellingShingle Other physical sciences not elsewhere classified
Solid state and materials
Physical Sciences not elsewhere classified
Shahd A.A. Alfadhli
Feodor Kusmartsev
Sergey Saveliev
Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields
title Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields
title_full Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields
title_fullStr Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields
title_full_unstemmed Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields
title_short Manipulating the anisotropy of the Dirac-Cone in graphene by laser fields
title_sort manipulating the anisotropy of the dirac-cone in graphene by laser fields
topic Other physical sciences not elsewhere classified
Solid state and materials
Physical Sciences not elsewhere classified
url https://hdl.handle.net/2134/37660