We probe the resistive switching response of Au/TiO2/Cu junctions, on samples initialized using both polarities electroforming. A conductive path is formed in both cases: a copper metallic filament for negative electroforming and a titanium dioxide possibly Magneli phase based filament for the positive case. We measured the resistance response of formed samples and studied their remanent resistance states. Bi (tri) stable resistance states were obtained for negative (positive) electroformed samples. The temperature dependence of the resistance discloses the underlying different nature of the associated filaments. In addition, we performed ab initio calculations to estimate the observed electroforming threshold voltages.

1.
G. I.
Meijer
,
Science
319
,
1625
(
2008
).
2.
A.
Sawa
,
Mater. Today
11
,
28
(
2008
).
3.
R.
Waser
,
R.
Dittmann
,
G.
Staikov
, and
K.
Szot
,
Adv. Mater.
21
,
2632
(
2009
).
4.
J. J.
Yang
,
I. H.
Inoue
,
T.
Mikolajick
, and
C. S.
Hwang
,
MRS Bull.
37
,
131
(
2012
).
5.
C.
Nauenheim
, in
8th IEEE Conference on Nanotechnology (NANO’08)
(
2008
), Vol.
464
, pp.
534
537
.
6.
J. J.
Yang
,
D. B.
Strukov
, and
D. R.
Stewart
,
Nat. Nanotechnol.
8
,
13
(
2013
).
7.
D. S.
Jeong
,
H.
Schroeder
, and
R.
Waser
,
Electrochem. Solid State Lett.
10
,
G51
G53
(
2007
).
8.
D. S.
Jeong
,
H.
Schroeder
, and
R.
Waser
,
Phys. Rev. B
79
,
195317
(
2009
).
9.
N.
Ghenzi
,
P.
Stoliar
,
M. C.
Fuertes
,
F. G.
Marlasca
, and
P.
Levy
,
Physica B
407
,
3096
(
2012
).
10.
I.
Valov
,
R.
Waser
,
J. R.
Jameson
, and
M. N.
Kozicki
,
Nanotechnology
22
,
254003
(
2011
).
11.
T.
Liu
,
M.
Verma
,
Y.
Kanga
, and
M. K.
Orlowskia
,
ECS Trans.
45
,
279
(
2012
).
12.
G. H.
Kim
,
J. H.
Lee
,
J. Y.
Seok
,
S. J.
Song
,
J. H.
Yoon
,
K. J.
Yoon
,
M. H.
Lee
,
K. M.
Kim
,
H. D.
Lee
,
S. W.
Ryu
 et al,
Appl. Phys. Lett.
98
,
262901
(
2011
).
13.
N.
Ghenzi
,
D.
Rubi
,
E.
Mangano
,
G.
Giménez
,
P.
Stoliar
, and
P.
Levy
,
Thin Solid Films
550
,
683
(
2014
).
14.
Y. B.
Nian
,
J.
Strozier
,
N. J.
Wu
,
X.
Chen
, and
A.
Ignatiev
,
Phys. Rev. Lett.
98
,
146403
(
2007
).
15.
M. J.
Rozenberg
,
M. J.
Sánchez
,
R.
Weht
,
C.
Acha
,
F.
Gomez-Marlasca
, and
P.
Levy
,
Phys. Rev. B
81
,
115101
(
2010
).
16.
N.
Ghenzi
,
M. J.
Sánchez
,
F. G.
Marlasca
,
P.
Levy
, and
M. J.
Rozenberg
,
J. Appl. Phys.
107
,
093719
(
2010
).
17.
F. G.
Marlasca
,
N.
Ghenzi
,
P.
Stoliar
,
M. J.
Sánchez
,
M. J.
Rozenberg
,
A. G.
Leyva
, and
P.
Levy
,
Appl. Phys. Lett.
98
,
123502
(
2011
).
18.
N.
Ghenzi
,
M. J.
Sánchez
,
M. J.
Rozenberg
,
P.
Stoliar
,
F. G.
Marlasca
,
D.
Rubi
, and
P.
Levy
,
J. Appl. Phys.
111
,
084512
(
2012
).
19.
N.
Ghenzi
,
M. J.
Sánchez
, and
P.
Levy
,
J. Phys. D: Appl. Phys.
46
,
415101
(
2013
).
20.
K.
Tsunoda
,
Y.
Fukuzumi
,
J. R.
Jameson
,
Z.
Wang
,
P. B.
Griffin
, and
Y.
Nishi
,
Appl. Phys. Lett.
90
,
113501
(
2007
).
21.
Y.
Kang
,
M.
Verma
,
T.
Liu
, and
M. K.
Orlowski
,
ECS Solid State Lett.
1
,
Q48
(
2012
).
22.
T.
Nagata
,
M.
Haemori
,
Y.
Yamashita
,
H.
Yoshikawa
,
Y.
Iwashita
,
K.
Kobayashi
, and
T.
Chikyow
,
Appl. Phys. Lett.
99
,
223517
(
2011
).
23.
K. J.
Yoon
,
M. H.
Lee
,
G. H.
Kim
,
S. J.
Song
,
J. Y.
Seok
,
S.
Han
,
J. H.
Yoon
,
K. M.
Kim
, and
C. S.
Hwang
,
Nanotechnology
23
,
185202
(
2012
).
24.
L.
Yang
, “
Resistive switching in TiO2 thin films
,” Ph.D. thesis (
JARA, Julich, Germany
,
2010
).
25.
F.
Yuan
,
J.
Wang
,
Z.
Zhang
,
Y.
Ye
,
L.
Pan
,
J.
Xu
, and
C. S.
Lai
,
Appl. Phys. Express
7
,
024204
(
2014
).
26.
D. H.
Kwon
,
K. M.
Kim
,
J. H.
Jang
,
J. M.
Jeon
,
M. H.
Lee
,
G. H.
Kim
,
X. S.
Li
,
G. S.
Park
,
B.
Lee
,
S.
Han
 et al,
Nat. Nanotechnol.
5
,
148
(
2010
).
27.
S. J.
Song
,
J. Y.
Seok
,
J. H.
Yoon
,
K. M.
Kim
,
G. H.
Kim
,
M. H.
Lee
, and
C. S.
Hwang
,
Sci. Rep.
3
,
3443
(
2013
).
28.
T.
Yanagida
,
K.
Nagashima
,
K.
Oka
,
M.
Kanai
,
A.
Klamchuen
,
B. H.
Park
, and
T.
Kawai
,
Sci. Rep.
3
,
1657
(
2013
).
29.
M. C.
Urdaniz
,
M. A.
Barral
, and
A. M.
Llois
,
Phys. Rev. B
86
,
245416
(
2012
).
30.
P.
Blaha
,
Wien2k, an Augmented Plane Wave Plus Local Orbitals Program for Calculating Crystal Properties
, edited by
K.
Schwarz
(
Technische Universität Wien
,
Austria
,
2001
).
31.
For the FP-LAPW calculations we used the GGA exchange and correlation potential, and parameters RKmax=6, 50 K points and muffin tin radii reduced so that they would not touch at the barrier top.
32.
See supplementary material at http://dx.doi.org/10.1063/1.4875559 for details of ab initio calculations.
33.
H.
Iddir
,
S.
Ogut
,
P.
Zapol
, and
N.
Browning
,
Phys. Rev. B
75
,
073203
(
2007
).
34.
M.
Weissmann
and
R.
Weht
,
Phys. Rev. B
84
,
144419
(
2011
).

Supplementary Material

You do not currently have access to this content.