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Copyright © 2010 American Scientific Publishers
All rights reserved
Printed in the United States of America
Journal of
Nanoscience and Nanotechnology
Vol. 10, 3562–3565, 2010
Local Structural and Optical Properties of
ZnO Nanoparticles
Eun-Suk Jeong
1
, Hyo-Jong Yu
1
, Yong-Jin Kim
2
, Gyu-Chul Yi
3
,
Yong-Dae Choi
4
, and Sang-Wook Han
1 ∗
1
Division of Science Education, Institute of Fusion Science, and Institute of Science Education,
Chonbuk National University, Jeonju 561-756, Korea
2
Department of Materials Science and Engineering, Pohang University of Science and
Technology, Pohang 790-784, Korea
3
National CRI Center for Semiconductor Nanorods and Department of Physics, Seoul National University,
Seoul 151-742, Korea
4
Department of Techno-Marketing, Mokwon University, Daejeon 302-718, Korea
This study examined the local structural and optical properties of ZnO nanoparticles (NPs) with
mean diameters of 4.5 and 70 nm using extended X-ray absorption fine structure (EXAFS) mea-
surements at the Zn K edge and photoluminescence (PL) measurements. EXAFS revealed that the
average bond length of atomic pairs in the NPs was shorter than that of the powder. Furthermore,
a substantial amount of structural disorder existed in the NPs. From the PL measurements, we
observed the direct band gap peak of 3.41 eV from the 70 nm ZnO NPs at low temperatures. This
blue shift was related to the structural property changes.
Keywords: EXAFS, Nanoparticle, ZnO, Structure, Photoluminescence, Quantum Confinement.
1. INTRODUCTION
ZnO nanostructures have been studied extensively for pos-
sible practical applications to nanometer-scale electronics
and photonics including transistors, gas sensors, light emit-
ting diodes (LEDs), ultra-violet (UV) sensors, piezoelec-
tric applications, biosensors, and field emission devices.
Recently, researchers have paid considerable attention to
ZnO nanoparticles for their quantum confinement effects.
Many studies reported observations of a quantum confine-
ment effect of ZnO nanoparticles (NPs)
1–4
and nanowires
5
using photoluminescence (PL) and Raman scattering mea-
surements. The previous studies reported that the ZnO
free exciton recombination peak was shifted from 3.3 eV
to ∼3.4 eV at low temperatures, as the ZnO NPs reduced
to a few nanometers. This blue shift was attributed to
the quantum confinement effect. However, the particle size
was still much larger than the Bohr radius of ZnO, which
is approximately 1.5 nm. The blue shift was even observed
from the ZnO nanoparticles (NPs) with a mean diameter of
more than 10 nm.
3 4
The blue shift could be attributed to a
structural change because the energy band gap can be engi-
neered by controlling the lattice constants of crystals.
6–8
∗
Author to whom correspondence should be addressed.
This study compared the local structural and the opti-
cal properties of NPs. Field-emission tunneling electron
microscopy (FE-TEM) is used to observe the atomic
arrangement in certain areas. However, it has limited res-
olution and cannot detect a small amount of lattice dis-
tortion. X-ray diffraction (XRD) is a powerful tool for
investigating the structures of crystalline materials but has
limitations when examining nanomaterials due to a small
number of scattering sources. Extended X-ray absorption
fine structure (EXAFS) can reveal the bond lengths, the
disorder of the bond lengths from a probe atom, the coordi-
nation numbers, and the species of the atoms.
9
Therefore,
EXAFS was used to quantify the local structural proper-
ties of ZnO NPs with an average particle size of 4.5 and
70 nm.
2. EXPERIMENTAL DETAILS
ZnO NPs, with two different sizes as shown in Figure 1,
were fabricated with a solution process.
10
Zinc acetate in
ethanol was boiled at approximately 80
C in air while
vigorously stirring. In an ultrasonic bath, ZnO NPs were
synthesized by supplying OH ions of lithium hydroxide
into the zinc-ethanol solution at approximately 0
C. The
3562 J. Nanosci. Nanotechnol. 2010, Vol. 10, No. 5 1533-4880/2010/10/3562/004 doi:10.1166/jnn.2010.2334