Available online at www.sciencedirect.com
Journal of the European Ceramic Society 30 (2010) 365–368
Development of PLZT dielectrics on base metal foils for
embedded capacitors
U. Balachandran
∗
, D.K. Kwon
1
, M. Narayanan, B. Ma
Energy Systems Division, Argonne National Laboratory, Argonne, IL 60439, United States
Available online 2 June 2009
Abstract
We have deposited Pb
0.92
La
0.08
Zr
0.52
Ti
0.48
O
3
(PLZT) films on nickel and copper substrates to create film-on-foil capacitors that exhibit excellent
dielectric properties and superior breakdown strength. Measurements with PLZT films on LaNiO
3
-buffered Ni foils yielded the following: relative
permittivity of 1300 (at 25
◦
C) and 1800 (at 150
◦
C), leakage current density of 6.6 × 10
-9
A/cm
2
(at 25
◦
C) and 1.4 × 10
-8
A/cm
2
(at 150
◦
C), and
mean breakdown field strength ≈2.5 MV/cm. With PLZT deposited directly on Cu foils, we observed dielectric constant ≈1100, dielectric loss
(tan δ) ≈0.06, and leakage current density of 7.3 × 10
-9
A/cm
2
when measured at room temperature.
© 2009 Elsevier Ltd. All rights reserved.
Keywords: Ferroelectric film; PLZT; Dielectric property; Chemical solution deposition
1. Introduction
The development of power electronic devices with improved
performance, increased reliability, small size, and reduced
weight requires the passive components to be embedded within a
printed wire board (PWB). This technology could free up surface
space, increase device reliability, and minimize electromag-
netic interference and inductance loss. Although the technology
has primarily received attention for decoupling capacitors in
microelectronic applications,
1–3
it can also be extended to high-
power applications at higher voltages, such as plug-in hybrid
electric vehicles. However, the integration of high-permittivity
films into PWBs is a difficult task because of the incompat-
ibility in the processing conditions for the different materials
involved. Polymer layers in a PWB cannot withstand the high
temperatures (600–800
◦
C) required for processing the ceramic
The submitted manuscript has been created by UChicago Argonne, LLC,
Operator of Argonne National Laboratory (“Argonne”). Argonne, a U.S. Depart-
ment of Energy Office of Science laboratory, is operated under Contract No.
DE-AC02-06CH11357. The U.S. Government retains for itself, and others act-
ing on its behalf, a paid-up nonexclusive, irrevocable worldwide license in said
article to reproduce, prepare derivative works, distribute copies to the public,
and perform publicly and display publicly, by or on behalf of the government.
∗
Corresponding author. Tel.: +1 630 252 4250; fax: +1 630 252 3604.
E-mail address: balu@anl.gov (U. Balachandran).
1
Current address: Materials Engineering Department, Korea Aerospace Uni-
versity, Gyeonggi-do, Korea.
film dielectrics to obtain the desired crystalline structures.
Development of these crystalline structures becomes extremely
challenging at reduced processing temperatures.
4
However, suc-
cess has been demonstrated through a film-on-foil approach
where the ceramic dielectrics are first coated on a thin base
metal foil by chemical solution deposition and then crystallized
at high temperature.
5–10
These coated foils can subsequently
be embedded into a PWB. Kingon and Srinivasan
5
reported
the deposition of PZT (52/48) films directly on copper foils
using a complex heat-treatment process and obtained dielectric
constant of ≈1100 and loss <5%. Maria et al.
7
reported fab-
rication of PLZT (15/52/48) on nickel plated copper foils that
achieved capacitance density of 350 nF/cm
2
and loss of 2%.
Zou et al.
8
reported growth of PZT on various metal substrates
and observed dielectric constant up to ≈450. In this paper, we
report our recent results on the dielectric properties of PLZT
film capacitors deposited on nickel and copper foils.
2. Experiment
Prior to being coated, the base metal (Ni or Cu) substrates
were polished with diamond paste to 1-m finish, ultrasonically
cleaned in distilled water, and then wipe-cleaned with acetone
and methanol using Texwipe Alpha swabs. LaNiO
3
(LNO) and
Pb
0.92
La
0.08
Zr
0.52
Ti
0.48
O
3
(PLZT 8/52/48) precursor solutions
were prepared by a modified 2-methoxyethanol synthesis route.
8
Detailed experimental conditions were reported earlier.
9
For
0955-2219/$ – see front matter © 2009 Elsevier Ltd. All rights reserved.
doi:10.1016/j.jeurceramsoc.2009.05.006