The transport properties of the devices made by corrugated graphene nanoribbons were investigated using the density functional theory in combination with the nonequilibrium Green’s function method. We find that the transport properties of the zigzag graphene nanoribbons (ZGNRs) with arched corrugation are similar to the flat one, while the transmission of the ZGNRs with step-shaped corrugation is greatly depressed. As for the armchair graphene nanoribbons (AGNRs), arched corrugation enlarges the transmission gap and the threshold voltage of the device. Moreover, the open currents of AGNRs are significantly depressed by both stepped and arched corrugation.

1.
K. S.
Novoselov
,
A. K.
Geim
,
S. V.
Morozov
,
D.
Jiang
,
Y.
Zhang
,
S. V.
Dubonos
,
I. V.
Grigorieva
, and
A. A.
Firsov
,
Science
306
,
666
(
2004
).
2.
C.
Berger
,
Z.
Song
,
X.
Li
,
X.
Wu
,
N.
Brown
,
C.
Naud
,
D.
Mayou
,
T.
Li
,
J.
Hass
,
A. N.
Marchenkov
,
E. H.
Conrad
,
P. N.
First
, and
W. A.
de Heer
,
Science
312
,
1191
(
2006
).
3.
M.
Ishigami
,
J. H.
Chen
,
W. G.
Cullen
,
M. S.
Fuhrer
, and
E. D.
Williams
,
Nano Lett.
7
,
1643
(
2007
).
4.
K.
Nomura
and
A. H.
MacDonald
,
Phys. Rev. Lett.
96
,
256602
(
2006
).
5.
Y.
Zhang
,
Y. -W.
Tan
,
H. L.
Stormer
, and
P.
Kim
,
Nature (London)
438
,
201
(
2005
).
6.
J.
Wu
,
W.
Pisula
, and
K.
Mullen
,
Chem. Rev.
107
,
718
(
2007
).
7.
X.
Wang
,
X.
Li
,
L.
Zhang
,
Y.
Yoon
,
P. K.
Weber
,
H.
Wang
,
J.
Guo
, and
H.
Dai
,
Science
324
,
768
(
2009
).
8.
J. C.
Meyer
,
A. K.
Geim
,
M. I.
Katsnelson
,
K. S.
Novoselov
,
T. J.
Booth
, and
S.
Roth
,
Nature (London)
446
,
60
(
2007
).
9.
A.
Fasolino
,
J. H.
Los
, and
M. I.
Katsnelson
,
Nat. Mater.
6
,
858
(
2007
).
10.
V. V.
Cheianov
and
V. I.
Fal’ko
,
Phys. Rev. Lett.
97
,
226801
(
2006
).
11.
M.
Katsnelson
and
A.
Geim
,
Philos. Trans. R. Soc. London
366
,
195
(
2008
).
12.
L.
Sun
,
Q.
Li
,
H.
Ren
,
H.
Su
,
Q. W.
Shi
, and
J.
Yang
,
J. Chem. Phys.
129
,
074704
(
2008
).
13.
O.
Hod
and
G. E.
Scuseria
,
Nano Lett.
9
,
2619
(
2009
).
14.
G. Q.
Li
,
J.
Cai
,
J. K.
Deng
,
A. R.
Rocha
, and
S.
Sanvito
,
Appl. Phys. Lett.
92
,
163104
(
2008
).
15.
G.
Kresse
and
J.
Hafner
,
Phys. Rev. B
49
,
14251
(
1994
).
16.
G.
Kresse
and
J.
Furthmüller
,
Phys. Rev. B
54
,
11169
(
1996
).
17.
J. P.
Perdew
and
Y.
Wang
,
Phys. Rev. B
45
,
13244
(
1992
).
18.
Z.
Li
,
H.
Qian
,
J.
Wu
,
B. -L.
Gu
, and
W.
Duan
,
Phys. Rev. Lett.
100
,
206802
(
2008
).
19.
M.
Brandbyge
,
J. -L.
Mozos
,
P.
Ordejón
,
J.
Taylor
, and
K.
Stokbro
,
Phys. Rev. B
65
,
165401
(
2002
)
. The double ζ plus polarization numerical orbital basis set was used for our systems. The exchange and correlation potential was approximated by GGA with PBE functional;
J. P.
Perdew
,
K.
Burke
, and
M.
Ernzerhof
,
Phys. Rev. Lett.
77
,
3865
(
1996
).
[PubMed]
20.
See supplementary material at http://dx.doi.org/10.1063/1.3419821 for the test of the choice of the exchange and correlation functional.

Supplementary Material

You do not currently have access to this content.