We used pulsed laser deposition to grow a series of PbTiO3/PbZr0.2Ti0.8O3 superlattices on SrTiO3 and SrRuO3/SrTiO3 substrates. An a/c polydomain structure was evidenced by reciprocal space mapping and by transmission electron microscopy. Insertion of ultra-thin layers of SrTiO3 at the interfaces between PbTiO3 and PbZr0.2Ti0.8O3 layers has inhibited this polydomain formation. A strong decrease in the tetragonality indicates clearly that the polarization state in these superlattices has changed due to the insertion of the SrTiO3 layers. A purely elastic mechanism does not seem to explain the determined structural parameters.

1.
D. G.
Schlom
,
L. Q.
Chen
,
C. B.
Eom
,
K. M.
Rabe
,
S. K.
Streiffer
, and
J. M.
Triscone
,
Annu. Rev. Mater. Res.
37
,
589
(
2007
).
2.
N. A.
Pertsev
,
V. G.
Kukhar
,
H.
Kohlstedt
, and
R.
Waser
,
Phys. Rev. B
67
,
054107
(
2003
).
3.
Q. Y.
Qiu
,
R.
Mahjoub
,
S. P.
Alpay
, and
V.
Nagarajan
,
Acta Mater.
58
,
823
(
2010
).
4.
Z.
Wu
and
R. E.
Cohen
,
Phys. Rev. Lett.
95
,
037601
(
2005
).
5.
G.
Catalan
,
A.
Janssens
,
G.
Rispens
,
S.
Csiszar
,
O.
Seeck
,
G.
Rijnders
,
D. H. A.
Blank
, and
B.
Noheda
,
Phys. Rev. Lett.
96
,
127602
(
2006
).
6.
A. H. G.
Vlooswijk
,
B.
Noheda
,
G.
Catalan
,
A.
Janssens
,
B.
Barcones
,
G.
Rijnders
,
D. H. A.
Blank
,
S.
Venkatesan
,
B.
Kooi
, and
J. T. M.
de Hosson
,
Appl. Phys. Lett.
91
,
112901
(
2007
).
7.
N.
Lemée
,
E.
Dooryhee
,
H.
Bouyanfif
,
F.
Le Marrec
,
M.
Nemoz
,
J. L.
Hodeau
, and
M. G.
Karkut
,
Phys. Rev. B
78
,
140102
(
2008
).
8.
F.
Le Marrec
,
R.
Farhi
,
M.
El Marssi
,
J. L.
Dellis
,
M. G.
Karkut
, and
D.
Ariosa
,
Phys. Rev. B
61
,
R6447
(
2000
).
9.
M.
Dawber
,
N.
Stucki
,
C.
Lichtensteiger
,
S.
Gariglio
,
P.
Ghosez
, and
J.-M.
Triscone
,
Adv. Mater.
19
,
4153
(
2007
).
10.
S.
Venkatesan
,
A.
Vlooswijk
,
B. J.
Kooi
,
A.
Morelli
,
G.
Palasantzas
,
J. T. M.
De Hosson
, and
B.
Noheda
,
Phys. Rev. B
78
,
104112
(
2008
).
11.
P.-E.
Janolin
,
B.
Fraisse
,
F.
Le Marrec
, and
B.
Dkhil
,
Appl. Phys. Lett.
90
,
212904
(
2007
).
12.
Here, monodomain refers to the case where only 180° domains exist and polydomains refers to the existence of both 180° and 90° domains.
13.
D.
Kuscer
,
J.
Holc
,
M.
Kosec
, and
A.
Meden
,
J. Am. Ceram. Soc.
89
,
3081
(
2006
).
14.
G.
Koster
,
B. L.
Kropman
,
G. J. H. M.
Rijnders
,
D. H. A.
Blank
, and
H.
Rogalla
,
Appl. Phys. Lett.
73
,
2920
(
1998
).
15.
A.
Boulle
,
O.
Masson
,
R.
Guinebretière
,
A.
Lecomte
, and
A.
Dauger
,
J. Appl. Crystallogr.
35
,
606
(
2002
).
16.
The samples were prepared at Institut d’Electronique, de Microélectronique et de Nanotechnologie (IEMN) of Lille (France) and at the Department of Physics and Astronomy, University of Glasgow (Scotland).
17.
I.
Vrejoiu
,
Y.
Zhu
,
G.
Le Rhun
,
M. A.
Schubert
,
D.
Hesse
, and
M.
Alexe
,
Appl. Phys. Lett.
90
,
072909
(
2007
).
18.
N. A.
Pertsev
and
A. G.
Zembilgotov
,
J. Appl. Phys.
78
,
6170
(
1995
).
19.
H. N.
Lee
,
H. M.
Christen
,
M. F.
Chisholm
,
C. M.
Rouleau
, and
D. H.
Lowndes
,
Nature
433
,
395
(
2005
).
20.
L. E.
Shilkrot
,
D. J.
Srolovitz
, and
J.
Tersoff
,
Appl. Phys. Lett.
77
,
304
(
2000
).
21.
We point out that the a/c polydomain structure is also detected in PT/PZT 20-80 SLs grown on SrTiO3 buffered with SrRuO3.
22.
Concerning oxygen vacancies: we believe that they are not significantly present in the polydomain SLs since the dd// is, on average, equal to that of individual PT and PZT. In the monodomain SLs, the sharp decrease in dSL cannot be explained by oxygen defects alone.
You do not currently have access to this content.