The size dependence of the ferroelectric properties of BaTiO3 nanowires is studied from first principles. We show that the ferroelectric distortion along the wire axis disappears below a critical diameter of about 1.2nm. This disappearance is related to a global contraction of the unit cell resulting from low atomic coordinations at the wire surface. It is shown that a ferroelectric distortion can be recovered under appropriate tensile strain conditions.

1.
M. E.
Lines
and
A. M.
Glass
,
Principles and Applications of Ferro-electrics and Related Materials
(
Clarendon
,
Oxford
,
1977
).
2.
C. H.
Ahn
,
K. M.
Rabe
, and
J.-M.
Triscone
,
Science
303
,
488
(
2004
).
3.
T.
Tybell
,
C. H.
Ahn
, and
J.-M.
Triscone
,
Appl. Phys. Lett.
75
,
856
(
1999
).
4.
D. D.
Fong
,
G. B.
Stephenson
,
S. K.
Streiffer
,
J. A.
Eastman
,
O.
Auciello
,
P. H.
Fuoss
, and
C.
Thompson
,
Science
304
,
1650
(
2004
).
5.
W. S.
Yun
,
J. J.
Urban
,
Q.
Gu
, and
H.
Park
,
Nano Lett.
2
,
447
(
2002
).
6.
Y.
Luo
,
I.
Szafraniak
,
N.
Zakharov
,
V.
Nagarajan
,
M.
Steinhart
,
R. B.
Wehrspohn
,
J. H.
Wendorff
,
R.
Ramesh
, and
M.
Alexe
,
Appl. Phys. Lett.
83
,
449
(
2003
).
7.
F. D.
Morrison
,
L.
Ramsay
, and
J. F.
Scott
,
J. Phys.: Condens. Matter
15
,
L527
(
2003
).
8.
M. W.
Chu
,
I.
Szafraniak
,
R.
Scholz
,
C.
Harnagea
,
D.
Hesse
,
M.
Alexe
, and
U.
Gösele
,
Nat. Mater.
3
,
87
(
2004
).
9.
Ph.
Ghosez
and
J.
Junquera
, in “
Handbook of Theoretical and Computational Nanotechnology
,” edited by
M
Rieth
and
W.
Schommers
(
ASP
, Stevenson Ranch, CA,
2006
), Vol. 7, p. 134.
10.
J.
Junquera
and
Ph.
Ghosez
,
Nature (London)
422
,
506
(
2003
).
11.
M.
Dawber
,
K. M.
Rabe
, and
J. F.
Scott
,
Rev. Mod. Phys.
77
,
1083
(
2005
).
12.
I.
Kornev
,
H.
Fu
, and
L.
Bellaiche
,
Phys. Rev. Lett.
93
,
196104
(
2004
).
13.
H.
Fu
and
L.
Bellaiche
,
Phys. Rev. Lett.
91
,
257601
(
2003
).
14.
I.
Naumov
,
H.
Fu
, and
L.
Bellaiche
,
Nature (London)
432
,
737
(
2004
).
15.
M. G.
Stachiotti
,
Appl. Phys. Lett.
84
,
251
(
2004
).
16.

Similar calculations were performed for selected nonstoichiometric wires with full Ba–O and full TiO2 coverage, yielding results similar to Fig. 2 except that the crossing between ac and a0 curves was slightly shifted to larger (respectively, smaller) cell parameters for BaO (respectively, TiO2) coverage.

17.
J. M.
Soler
,
E.
Artacho
,
J.
Gale
,
A.
Garcia
,
J.
Junquera
,
P.
Ordejón
, and
D.
Sánchez-Portal
,
J. Phys.: Condens. Matter
14
,
2745
(
2002
).
18.
J.
Junquera
,
M.
Zimmer
,
P.
Ordejón
, and
Ph.
Ghosez
,
Phys. Rev. B
67
,
155327
(
2003
).
19.
X.
Gonze
,
J.-M.
Beuken
,
R.
Caracas
,
F.
Detraux
,
M.
Fuchs
,
G.-M.
Rignanese
,
L.
Sindic
,
M.
Verstraete
,
G.
Zerah
,
F.
Jollet
,
M.
Torrent
,
A.
Roy
,
M.
Mikami
,
Ph.
Ghosez
,
J.-Y.
Raty
, and
D. C.
Allan
,
Comput. Mater. Sci.
25
,
478
(
2002
);
20.

To test the possible influence (especially in reason of the lateral dipole) of the artificial replica induced by the periodic boundary conditions, we repeated some calculations enlarging the vacuum regions up to 20Å, without significant change in the results.

21.
R. D.
King-Smith
and
D.
Vanderbilt
,
Phys. Rev. B
47
,
1651
(
1993
).
22.
D.
Sánchez-Portal
,
I.
Souza
, and
R. M.
Martin
, in
Fundamental Physics of Ferroelectrics 2000
, AIP Conf. Proc.
535
, edited by
R. E.
Cohen
(
AIP
,
Melville, NY
,
2000
), p.
111
.
23.

The Born effective charges along z for the four Ti in a section of the wire of Fig. 1(c) are: ZTi1*=5.10, ZTi2*=5.78, ZTi3*=5.93 [labels as in Fig. 1(d)].

24.
J.
Padilla
and
D.
Vanderbilt
,
Phys. Rev. B
56
,
1625
(
1997
).
25.
Ph.
Ghosez
,
X.
Gonze
, and
J.-P.
Michenaud
,
Ferroelectrics
206
,
205
(
1998
).
26.
Ph.
Ghosez
,
E.
Cockayne
,
U. V.
Waghmare
, and
K. M.
Rabe
,
Phys. Rev. B
60
,
836
(
1999
).
You do not currently have access to this content.