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IEEE TRANSACTIONS ON ELECTRON DEVICES 1
The Demonstration of High-Performance
Multilayer BaTiO
3
/BiFeO
3
Stack MIM Capacitors
Chin Lien , Cho-Fan Hsieh, Hung-Sen Wu, Teng-Chun Wu, Syu-Jhih Wei,
Yu-Heng Chu, Ming-Han Liao , and Min-Hung Lee
Abstract — Multilayer BaTiO
3
/BiFeO
3
(BTO/BFO) stack
structures were prepared on the Pt/TiO
2
/SiO
2
/Si (100) sub-
strate via highly accurate magnetron sputtering process.
The cubic to the tetragonal phase transition of BTO
was confirmed by both the X-ray diffraction and Raman
spectroscopy after the process of rapid thermal anneal.
An ∼74.1% increase of the relative permittivity was
observed with the increasing thickness of BFO in the
metal–insulator–metal capacitor. On the other hand, we
also demonstrate that the leakage current density and the
relative permittivity are found to have 20–50 times reduction
and 26.6% improvement, respectively, with the additional
cap of the BTO layer.
Index Terms— Barium titanate (BaTiO
3
, BTO), bismuth
ferrite (BiFeO
3
, BFO), metal–insulator–metal (MIM) capaci-
tor, multilayer stack, rapid thermal anneal (RTA).
I. I NTRODUCTION
C
APACITORS are widely used in portable, power, and
radio frequency (RF) electronics [1], [2]. Especially a
metal–insulator–metal (MIM) capacitor has become popular
because the metal electrodes provide depletion free and high
conductance nature, which are suitable for the high-speed
application. With the development of the scaling technology,
the requirements of MIM capacitors such as high capacitance
density with low-leakage current and good compatibility of the
miniaturizing circuit design should be met. In the past decades,
many scientists focused on developing high-k dielectrics such
as Al
2
O
3
[3], [4], Ta
2
O
5
[5], [6], ZrO
2
[7], and HfO
2
[8], [9]
Manuscript received July 26, 2018; accepted September 1, 2018. This
work was supported in part by the Department of Industrial Technology,
Ministry of Economic Affairs, Taiwan, in part by the Department of
Mechanical Engineering, National Taiwan University, and in part by
the National Device Laboratory supports the device fabrication and
measurement. The review of this paper was arranged by Editor B. Kaczer.
(Corresponding authors: Chin Lien; Ming-Han Liao.)
C. Lien, C.-F. Hsieh, H.-S. Wu, and T.-C. Wu are with the Center
of Measurement Standards, Industrial Technology Research Institute,
Hsinchu 31040, Taiwan (e-mail: clien@itri.org.tw).
S.-J. Wei, Y.-H. Chu, and M.-H. Liao are with the Department of
Mechanical Engineering, National Taiwan University, Taipei 10617,
Taiwan (e-mail: mhliaoa@ntu.edu.tw).
M.-H. Lee is with the Institute of Electro-Optical Science and Technol-
ogy, National Taiwan Normal University, Taipei 10610, Taiwan.
Color versions of one or more of the figures in this paper are available
online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TED.2018.2868849
which can be used as the dielectric layer in MIM capacitors.
However, permittivity (ε) and leakage current ( J g) are the
critical issues which would limit the usage of these high-k
dielectrics in the high-power circuit or the applications of
energy storage devices [10].
Thanks to the continuous development of material, bar-
ium titanate-based (BaTiO
3
, BTO) and bismuth ferrite-based
(BiFeO
3
, BFO) materials have been proposed to be used
as the dielectric layer in semiconductor devices since the
past decade [11], [12]. For example, some researchers have,
nowadays, observed the negative capacitance (NC) effect and
demonstrate its successful and useful application in the low
power emerging field-effect transistors (FETs) and memory
devices. The FETs with NC effect possess the lower operated
drain voltage (V
DD
), and the steeper subthreshold swing is
regarded as a potential candidate for the next-generation logic
devices [13]–[16].
A BTO with a spontaneous polarization associated with
the extremely high permittivity has a good breakdown
endurance [17], [18], which can be regarded as the poten-
tial candidate of capacitor dielectric in the next generation.
Unfortunately, even in the tetragonal phase, a small saturated
polarization of BTO limits its application on the energy storage
devices in the future. On the other hand, a BFO is found
to be as a nature multiferroic material, which exists two
ferroic orders including ferroelectric and antiferromagnetic at
the room temperature. High theoretical saturated polarization
(∼90 μC/cm
2
) implies more charges can be stored in this
kind of dielectric. In addition, a BFO has a ferroelectric
Curie temperature (T
C
) of 1103 K and antiferromagnetic Néel
temperature (T
N
) of 643 K, which are suitable to be used in
the high-temperature operation conditions [19]–[21]. However,
the high J g associated with poor ferroelectricity limit the pos-
sibility to use BFO only dielectric for the device applications.
In this paper, we proposed a novel MIM capacitor structure
with the multilayer BTO/BFO stack design. The tetragonal
phase of a BTO thin film was presented through a few seconds
rapid thermal anneal (RTA) process. The thickness of BFO thin
film and an additional cap of BTO film were investigated and
optimized to achieve the outstanding electrical characteristics
in our multilayer BTO/BFO MIM capacitors.
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