Quantum confinement effect of
ZnO nano-particles
Cao Li, Su Xiyu, Wu Zhenyu#,
Zou Bingsuo#, Dai Jiahua#, Xie Sishen#
(Department of Physics, Qufu Normal University, Qufu, Shandong, 273165; #Institute
of Physics, CAS, Beijing 100080 )
Received Mar.28, 2002.
Abstract Zinc oxide nanocrystals were prepared with different size and shape by coating of dodecyl benzene sulfonate (DBS) . Good evidences can
prove that quantum confinement effect is the special quality for this nanosystem. As an
indication of quantum confinement effect, excellent emissions from bandedge have been
observed, which is necessary for the laser nanodevices.
Keywords Quantum confinement effect, Zinc oxide, Nanocrystals.
1. INTRODUCTION
It is well known, nano-materials will find
more and more applications in the technological development in the future. As a typical
quantum solid, nano-semiconductor materials have more novel quality than their bulk
materials. II-VI semiconductor
materials, which have many new properties that attract both fundamental and technological
interests to many researchers today, such as solar cells [1-4], chemical
sensors [5-6], luminescent and electrical devices [7], and some
kinds of display units[8]. Among them, zinc oxide is one of useful materials
with optically active property. ZnO dots and wires in nano-scale span a wide range of
electrical and optical properties that depend sensitively on both size and shape. Quantum
confinement effect can modify the energy bands with the change of the size and shape of
the nano-particles. Many physical and chemical methods can be used to change the particles
size and shape, such as the control of the growth kinetics which is a good method to vary
the CdSe particles shapes from a nearly spherical morphology to a rod-like ones [9],
Dodecyl benzene sulfonate (DBS) and poly (vinylpyrrolidone) (PVP) are better stabilizers,
which can effectively change the morphology of zinc oxide nano-particles. For example,
many novel properties can be found through varying the molar ratio of the ion of Zn and
PVP, with this method, the rod shape particles are made, many optical properties are
observed [10].
Here we find another way to obtain the anisotropic nanocrystal of ZnO
by control the pH of microemulsion pool for the ZnO nanocrystal formation, quantum
confinement effects can be observed for the absorption and emission properties of this
system. Particles with different size and shape and their concrete changes about energy
band and optical phenomena are clearly presented.
2. EXPERIMENT
0.03mol zinc chloride (AR grade) were dissolved in 300mL deionized water. Then DBS
solution was added to form mixed solution. The HCl and NaOH solution were used to control
the pH value of this solution. Toluene was used as the extraction solvent to form the
organosol of Zn(OH)2 nanoparticles. To control the particle size and
shape, pH value of the mixed solution were adjusted from 3.5 to 5.8. In this pH range the
ZnO nanoparticles can be extracted into toluene easily. While pH>=6.2, it is hard to
form homogeneous micelle. When the coated ZnO was extracted, then it was refluxed at about
110ºC for 2-3hr and to remove
excess water. The size of ZnO organosol was detected by TEM of JEOL 2010, its electric
voltage is 200Kv and amplification multiple is 0.2 million; The TU-1901 UV-Visible
absorption spectrometer and PTI-C-70 fluorescence spectrometer were used to study the
absorption and emission of the samples.
3. RESULTS AND DISCUSSION
We have prepared zinc oxide nano-particles
with different shapes. Figure 1 is the TEM figure of the two different shape samples, a
rod-like one at high pH with above 10nm (a), and a sphere-like one at low pH (<4)
(4-5nm) (b). The TEM of ZnO nanoparticle with 1-2 nm has been reported elsewhere [11].
The rod-like one have the quality of one-dimension semiconductor material [2],
this can be verified by the following description.
Figure 2 is the change of
the energy bandgap with the size changing. From the figure we can find that the samples
with the different size have evident shift as shown. A significant blue shift of the
absorption edge compared to that of bulk ZnO in the absorption spectra is observed when
the particles' size decreases. This shift firmly
attests the theory of quantum confinement effect. Quantum confinement effect can be
described with the Brus formula
[12]:
(a) (b)
Fig.1 The TEM photographs of
the ZnO nano-particles with different size and shape. From the figure we know that we can
prepare the shape we needed.
Where is the
absorption band gap of nano-semiconductor particles, is the bulk ZnO band gap energy, r
is the radius of the parcicle,is
the exciton reduced mass , where and
are the effective masses of the electron and hole ,e*=e0/e1
is the relative dielectric constant, where e0
and e1 is the dielectric constants of the bulk ZnO and the
capping DBS), , which is the Rydberg energy.
Generally, it is accepted that the relative dielectric constant e*=2.47 and the effective masses of an electron and a hole
expressed in free electron mass are 0.24 and 0.45 and the bulk band energy we used is 3.2eV in ZnO solid, the reference [13]
gave the units of 156 meV and the exciton
Bohr radius aB=1.25 nm.
Fig.2 The change of
the band gap energy Eg with the particle size. When
the particle size is in the range of nanometer, the
band energy increases with the size decreasing as the figure shown.
Evidently, from the
formula and Figure 2, we can see that the energy band change upwards, therefore optical
absorption and blue shift correspondingly with the size change.
Fig.3 A
clearly quantum confinement effect is provided, we can see from the absorption spectra
that the ZnO quantum dots (~2nm,5nm,>10nm) we have provided can give a good description
about the absorption spectra band blue-shifting following the particles size decreasing, at the same time the exciton
absorption peak becomes more apparent and blue shift with the size decrease. Furthermore
it can be seen the exciton effect is evident when the size is decreased.
Fig.4 The fluorescence spectra of the nano-particles. (A) is excitation
spectra and (B) is the photoluminescence spectra. Excitation peak is at 360nm, and the
emission peak at 404nm (which is attributed to the electron hole recombination in the
band-gap).
With the
same coating, the inner and the cover have different dielectric constants, so the change
of nano-particles shape can bring about the following
change of the ground states of the bounded exciton in the nano-particles, the change of
the surface polarization effect acting on the bounded action of the exciton comes from the
discontinuousness of the dielectric constants. From the formula and Figure 2, we can find
that the deviation of the theoretical and the experimental values mainly come from the
second and the last term in the right part of the formula, because, theoretically, the
values we used are the bulk materials, including the effective mass of the electron, the
hole and the dielectric constant, furthermore we do not
think about the coating can affect the reduced mass of electron and hole. All of these are
the reasons that can affect the deviation.
As we all known, stronger exciton effect is an important character of
quantum confinement effect in nano-semiconductors, the reason mainly comes from the
carriers being confined in a very small district, this makes the electron and hole move
only in a potential well. At the same time, it can enhance the coupling interaction with
each other. Then the exciton bounded stronger and the probability of binding increased, so
we can observe more apparent exciton absorption peak when the particles' size decreased. Therefore we can see the exciton absorption and
their blueshifts in Fig.3.
Figure 4 is the fluorescence
spectra of the ZnO nano-particles. Curve A is the excitation spectrum and curve B is the
emission spectrum. The excitation peak is about 360nm and the value of the
photoluminescence peak is 404nm. Obviously, the band gap luminescence of ZnO nanocrystal
is predominant in the emission spectrum. The blue shift takes place when the values are
relative to the bulk samples and the enhancement of the bandedge resonant fluorescence
shows the contribution of the quantum confinement effect. Surface states are of importance
for radiative transitions for ZnO particles in the ref. [14-15], which is also the main
radiationless channel. The luminescence of ZnO is very sensitive to the surface states,
but the surface states can be controlled by the preparation methods, that is to say,
different preparation methods can lead to different optical phenomena [14-19].
In our system, the organic coating occupies the surface states and forms the surface
potential barrier, which can prevent the formation of the
surface states and hence the resonance radiation transition of the exciton dominates. This
property will be eventually applied in ZnO laser devices.
4. CONCLUSIONS
In conclusion, with the control of the pH of
the mixed microemulsion ZnO solution, nanocrystal with different size and shape are
prepared. Our results can be described in terms of the quantum confinement effect. The
better zinc oxide nano-particles with the good method of surface decoration have been
prepared, so our samples have no obvious surface states that lead to the quality
undesired. Therefore, this surface decoration can improve the emission property of ZnO,
which is very important for the developing high quality nano-devices.
Acknowledgments The authors
would like to thank National Natural Science Foundation of China (Term No 20173073) and
Hundred Talent Project of Chinese Academy of Science for the financial support.
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