Reproducible unipolar resistive switching behaviors in the metal-deficient CoO
x
thin film
June Sik Kwak
a
, Young Ho Do
a
, Yoon Cheol Bae
b
, Hyunsik Im
c
, Jin Pyo Hong
a,
⁎
a
Novel Functional Materials and Device Lab, Department of Physics, Hanyang University, Seoul 133-791, Republic of Korea
b
Department of Engineering of Nano Semiconductor, Hanyang University, Seoul 133-791, Republic of Korea
c
Department of Semiconductor Science, Dongguk University, Seoul 100-715, Republic of Korea
abstract article info
Available online xxxx
Keywords:
CoO
x
Resistive switching
Nonvolatile memory
ReRAM
Pt/CoO
x
/Pt tri-layers exhibited reproducible and stable unipolar switching under a dc sweeping voltage. In
order to investigate the role of oxygen reduction in the metal-deficient CoO
x
layer, resistive switching of the
post-annealed CoO
x
thin film was compared with those of the as-deposited CoO
x
thin film. X-ray
photoemission spectroscopy showed larger reproducible resistance switching and decreasing of current level
in the post-annealed CoO
x
thin film. This may be explained by a reduction in oxygen stoichiometry without
phase transformation of the CoO
x
. In addition, stable switching in post-annealed CoO
x
layer is considered to
originate from the decrease of the Co vacancies in local Co
3
O
4
region partially distributed in the whole CoO
x
layer, not in the dominant CoO.
© 2010 Elsevier B.V. All rights reserved.
1. Introduction
Resistive switching materials for next-generation nonvolatile
memory (NVM) were widely investigated in various oxide materials,
such as binary transition metal oxides (TMO) [1–11], perovskite
structure ternary oxides [12,13] and others. The resistive random
access memory (ReRAM) is based on the resistance switching effect
and is considered to be the most promising candidate for NVM due to
superior properties including simple structure, high density integra-
tion, high speed switching, and low power consumption. From a
practical point of view, binary TMOs are some of the most compatible
materials for ReRAM applications because of simply controllable
stoichiometry and compatibility with standard complementary
metal-oxide semiconductor technology (CMOS) [2,14–18].
Resistance switching in binary TMO thin films, such as NiO [1–4],
TiO
2
[5–8], HfO
2
[9], and CoO
x
[10,11], has been intensively studied in
terms of device properties and modeling of the resistive switching
mechanism. Although exact microscopic mechanisms are still under
discussion, the conductive filamentary paths model is generally
considered as a dominant switching mechanism in binary TMO
films. According to the filamentary path model, it is reasonable to
assume that the electro-migration of oxygen vacancies or metal
vacancies might play an important role in the generation and
annihilation of conductive filamentary paths [1,2,4–7,16,18]. There-
fore, the dependence of the vacancy characteristics will be an important
parameter in determining the resistance switching properties.
CoO is a rocksalt 3d transition metal monoxide with interesting
electrical properties. Theoretical calculations of ideally stoichiometric
CoO predict that it is a charge transfer insulator with a band gap of
approximately 2.4 eV [10,11]. However, because of non-stoichiome-
try, the CoO
x
thin film can become a p-type oxide with metal
deficiency [12]. Therefore, it is expected that the transport and
switching properties of CoO
x
can be controlled by varying oxygen
content in CoO
x
thin films. In this article, we investigate the resistive
switching properties of as-deposited CoO
x
and post-annealed CoO
x
films, as well as the effect of oxygen reduction during the post-
annealing process.
2. Experimental details
A Pt/CoO
x
/Pt metal–oxide–metal (MOM) structure was fabricated
as a resistance switching cell. The 100-nm-thick Pt layer and 30-nm-
thick Ti layer were prepared on SiO
2
/Si (100) substrate using dc
magnetron sputtering at room temperature, where the 30-nm-thick
Ti layer was deposited for adhesion. Subsequently, the 50-nm-thick
CoO
x
layer was deposited on the Pt electrode by radio frequency
sputtering using a Co–O target (99.95% pure) under an argon pressure
of 1 mTorr.
In order to investigate the resistance switching characteristics of
CoO
x
, 100-nm-thick Pt top electrodes were fabricated by a conven-
tional photolithography and lift-off process. The size of the top
electrode was patterned to be 50 μm×50 μm. Post-thermal annealing
at 400 °C was performed in an argon atmosphere using a rapid
thermal annealing (RTA) chamber for a few minutes. As a baseline
experiment, the valence state of Co in CoO
x
and in the post-annealed
CoO
x
layer was determined using KRATOS AXIS NOVA x-ray
Thin Solid Films xxx (2010) xxx–xxx
⁎ Corresponding author. Tel.: +82 2 2220 0911; fax: +82 2 2295 6868.
E-mail address: jphong@hanyang.ac.kr (J.P. Hong).
TSF-27307; No of Pages 4
0040-6090/$ – see front matter © 2010 Elsevier B.V. All rights reserved.
doi:10.1016/j.tsf.2010.03.050
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ARTICLE IN PRESS
Please cite this article as: J.S. Kwak, et al., Thin Solid Films (2010), doi:10.1016/j.tsf.2010.03.050