A scheme to produce closely spaced high-quality one-dimensional electronic channels is presented. It is based on standard nanolithography fabrication applied to a single, wide quantum well AlGaAs/GaAs heterostructure where the spatial separation of the wire modes is given by Coulomb repulsion. The lack of a composition-induced barrier in the double layer leads to electron mobility of 5×106cm2/Vs in the starting double two-dimensional system. This in turn yields high-quality one-dimensional channels following nanolithography, as shown by our detailed analysis of the magnetotransport properties of the system. Variable coupling is achieved by split-gate polarization and external magnetic-field intensity and orientation. The relevance for the implementation of coherent nanodevices of this fabrication approach is discussed.

1.
V.
Piazza
,
F.
Beltram
,
W.
Wegscheider
,
C.-T.
Liang
, and
M.
Pepper
,
Phys. Rev. B
62
,
10630
(
2000
).
2.
M. J.
Gilbert
and
J. P.
Bird
,
Appl. Phys. Lett.
77
,
1050
(
2000
).
3.
R.
Ionicioiu
,
P.
Zanardi
, and
F.
Rossi
,
Phys. Rev. A
63
,
050
101
(
2001
).
4.
A.
Bertoni
,
P.
Bordone
,
R.
Brunetti
,
C.
Jacoboni
, and
S.
Reggiani
,
Phys. Rev. Lett.
84
,
5912
(
2000
).
5.
K. J.
Thomas
,
J. T.
Nicholls
,
N. J.
Appleyard
,
M. Y.
Simmons
,
M.
Pepper
,
D. R.
Mace
,
W. R.
Tribe
, and
D. A.
Ritchie
,
Phys. Rev. B
58
,
4846
(
1998
);
C.-T.
Liang
,
M. Y.
Simmons
,
C. G.
Smith
,
D. A.
Ritchie
,
M.
Pepper
,
Appl. Phys. Lett.
75
,
2975
(
1999
).
6.
C.-T.
Liang
,
M.
Pepper
,
M. Y.
Simmons
,
C. G.
Smith
, and
D. A.
Ritchie
,
Phys. Rev. B
61
,
9952
(
2000
).
7.
K. S.
Pyshkin
,
C. J. B.
Ford
,
R. H.
Harrell
,
M.
Pepper
,
E. H.
Linfield
, and
D. A.
Ritchie
,
Phys. Rev. B
62
,
15
842
(
2000
).
8.
A.
Kristensen
,
H.
Bruus
,
A. E.
Hansen
,
J. B.
Jensen
,
P. E.
Lindelof
,
C. J.
Marckmann
,
J.
Nygård
,
C. B.
Sørensen
,
F.
Beuscher
,
A.
Forchel
, and
M.
Michel
,
Phys. Rev. B
62
,
10
950
(
2000
).
9.
Y.
Feng
,
A. S.
Sachrajda
,
P.
Zawadzki
,
S.
Kolind
,
M.
Buchanan
,
J. H.
Smet
,
J.
Lapointe
, and
P. A.
Marshall
,
J. Vac. Sci. Technol. A
18
(
2
),
730
(
2000
);
I. M.
Castleton
,
A. G.
Davies
,
A. R.
Hamilton
,
J. E. F.
Frost
,
M. Y.
Simmons
,
D. A.
Ritchie
, and
M.
Pepper
,
Physica B
251
,
157
(
1998
).
10.
C. C.
Eugster
and
J. A.
del Alamo
,
Phys. Rev. Lett.
67
,
3586
(
1991
);
C. C.
Eugster
,
J. A.
del Alamo
,
M. J.
Rooks
, and
M. R.
Melloch
,
Appl. Phys. Lett.
64
,
3157
(
1994
).
11.
K. J.
Thomas
,
J. T.
Nicholls
,
M. Y.
Simmons
,
W. R.
Tribe
,
A. G.
Davies
, and
M.
Pepper
,
Phys. Rev. B
59
,
12252
(
1999
).
12.
T. J.
Thornton
,
M.
Pepper
,
H.
Ahmed
,
D.
Andrews
, and
G. J.
Davies
,
Phys. Rev. Lett.
56
,
1198
(
1986
).
13.
B. J.
van Wees
,
H.
van Houten
,
C. W. J.
Beenakker
,
J. G.
Williamson
,
L. P.
Kouwenhoven
,
D.
van der Marel
, and
C. T.
Foxon
,
Phys. Rev. Lett.
60
,
848
(
1988
);
D. A.
Wharam
,
T. J.
Thornton
,
R.
Newbury
,
M.
Pepper
,
H.
Ahmed
,
J. E. F.
Frost
,
D. G.
Hasko
,
D. C.
Peacock
,
D. A.
Ritchie
, and
G. A. C.
Jones
,
J. Phys. C
21
,
L209
(
1988
).
14.
B. J.
van Wees
,
L. P.
Kouwenhoven
,
E. M. M.
Willems
,
C. J. P. M.
Harmans
,
J. E.
Mooij
,
H.
van Houten
,
C. W. J.
Beenakker
,
J. G.
Williamson
, and
C. T.
Foxon
,
Phys. Rev. B
43
,
12
431
(
1991
).
15.
The absence of the conductance step at G=5×2e2/h when all the lower steps are present, indicates a degeneracy condition between the first 1D subband in the higher-energy 2D layer and the fifth 1D subband in the lower-energy 2D layer. For Vg<−3.6V(G<5×2e2/h) only one electronic layer is populated and the steps are nearly equally spaced.
16.
V.
Piazza
,
V.
Pellegrini
,
F.
Beltram
,
W.
Wegscheider
,
T.
Jungwirth
, and
A. H.
MacDonald
,
Nature (London)
402
,
638
(
1999
).
17.
B.
Tanatar
,
I.
Al-Hayek
, and
M.
Tomak
,
Phys. Rev. B
58
,
9886
(
1998
).
18.
C.
Steinebach
,
D.
Heitmann
, and
V.
Gudmundsson
,
Phys. Rev. B
58
,
13
944
(
1998
).
19.
C. D.
Simserides
,
J. Phys.: Condens. Matter
11
,
5131
(
1999
).
This content is only available via PDF.
You do not currently have access to this content.