Optical properties of graphene antidot lattices
Publication: Research - peer-review › Journal article – Annual report year: 2008
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Optical properties of graphene antidot lattices. / Pedersen, Thomas Garm; Flindt, Christian; Pedersen, Jesper Goor; Jauho, Antti-Pekka; Mortensen, Asger; Pedersen, Kjeld.
In: Physical Review B (Condensed Matter and Materials Physics), Vol. 77, No. 24, 2008, p. 245431.Publication: Research - peer-review › Journal article – Annual report year: 2008
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TY - JOUR
T1 - Optical properties of graphene antidot lattices
A1 - Pedersen,Thomas Garm
A1 - Flindt,Christian
A1 - Pedersen,Jesper Goor
A1 - Jauho,Antti-Pekka
A1 - Mortensen,Asger
A1 - Pedersen,Kjeld
AU - Pedersen,Thomas Garm
AU - Flindt,Christian
AU - Pedersen,Jesper Goor
AU - Jauho,Antti-Pekka
AU - Mortensen,Asger
AU - Pedersen,Kjeld
PB - American Physical Society
PY - 2008
Y1 - 2008
N2 - Undoped graphene is semimetallic and thus not suitable for many electronic and optoelectronic applications requiring gapped semiconductor materials. However, a periodic array of holes (antidot lattice) renders graphene semiconducting with a controllable band gap. Using atomistic modeling, we demonstrate that this artificial nanomaterial is a dipole-allowed direct-gap semiconductor with a very pronounced optical-absorption edge. Hence, optical infrared spectroscopy should be an ideal probe of the electronic structure. To address realistic experimental situations, we include effects due to disorder and the presence of a substrate in the analysis.
AB - Undoped graphene is semimetallic and thus not suitable for many electronic and optoelectronic applications requiring gapped semiconductor materials. However, a periodic array of holes (antidot lattice) renders graphene semiconducting with a controllable band gap. Using atomistic modeling, we demonstrate that this artificial nanomaterial is a dipole-allowed direct-gap semiconductor with a very pronounced optical-absorption edge. Hence, optical infrared spectroscopy should be an ideal probe of the electronic structure. To address realistic experimental situations, we include effects due to disorder and the presence of a substrate in the analysis.
KW - SIO2
UR - http://link.aps.org/doi/10.1103/PhysRevB.77.245431
U2 - 10.1103/PhysRevB.77.245431
DO - 10.1103/PhysRevB.77.245431
JO - Physical Review B (Condensed Matter and Materials Physics)
JF - Physical Review B (Condensed Matter and Materials Physics)
SN - 1098-0121
IS - 24
VL - 77
SP - 245431
ER -