Materials Science and Engineering B 177 (2012) 1452–1459
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Materials Science and Engineering B
j o ur nal homep age: www.elsevier.com/locate/mseb
Structural and optical characterization of mechanochemically synthesized
copper doped CdS nanopowders
P. Reyes
∗
, S. Velumani
Departamento de Ingeniería Eléctrica-SEES, CINVESTAV-IPN, Zacatenco, D.F., C.P.07360, México, Mexico
a r t i c l e i n f o
Article history:
Received 1 October 2011
Received in revised form 18 February 2012
Accepted 3 March 2012
Available online 28 March 2012
Keywords:
Cu doped CdS
Ball milling
Nanopowder
HRTEM
a b s t r a c t
Incorporation of copper into CdS crystals has been successfully prepared by mechanical alloying using
a planetary ball mill. The powders are prepared with different milling times at 300 rpm with various
Cu/Cd ratios from 0.1 to 25 at%. X-ray diffraction (XRD) analysis of milled powders showed peaks corre-
sponding to hexagonal structure with a detection of phase transition to a cubic structure with increasing
milling time. Grain sizes varied from 21 to 30 nm corresponding to different Cu/Cd ratios. Field emis-
sion scanning electron microscopy (FESEM) images reveal agglomerated materials with particle size of
approximately 28 nm (5 Cu at%) and layered structures caused due to the milling process. Powder com-
position by energy dispersive analysis of X-rays (EDAX) reveals the incorporation of copper into the CdS.
Micro Raman spectroscopy showed peaks approximately at 301 and 585 cm
-1
corresponding to first and
second order scatterings of longitudinal optical phonon mode. The LO mode at 301 cm
-1
shifted towards
lower wave number due to decrease of grain size by increase in milling time. From high resolution trans-
mission electron microscope (HRTEM), the dominant phase of individual CdS nanocrystals was found to
be hexagonal structure along with cubic structure.
© 2012 Elsevier B.V. All rights reserved.
1. Introduction
CdS is a II–VI n-type semiconductor with a direct band-gap of
2.42 eV and a hexagonal (stable) or cubic (metastable) structure. It
has applications in laser materials, photo resistance, light emitting
diode, nonlinear optical devices, etc. It is widely used as window
material for solar cells [1]. Two basic requirements for the window
material are the low electrical resistivity and high optical transmit-
tance. An effective way to obtain CdS with these requirements can
be achieved by the creation of Cd excess or S vacancies [2] with the
incorporations of different impurities such as Cu [3], Fe [4] Ag [5],
Al [6] and Ga [7]. Copper impurities behave as an acceptor in CdS,
changing the resistivity, bandgap energy, photoelectrical proper-
ties [3] and also changing the type of semiconductor from n to p
(useful for CdS:Cu/CdS PV devices) [3].
Many methods have been used to incorporate dopants into CdS,
some of these methods are: ion-exchange reaction [8], dry process
[9], spray pyrolysis [10], and vacuum deposition [11]. Mechani-
cal alloying (MA) can be considered as a simple, inexpensive and
novel alternate process to obtain CdS with various Cu concen-
trations. MA is a solid-state processing technique that involves
welding, fracturing and rewelding of powder particles at atomic
∗
Corresponding author. Tel.: +52 55 5747 4001; fax: +52 55 5747 4003.
E-mail addresses: pireyes@cinvestav.mx, itzam29@gmail.com (P. Reyes).
level [12], capable of synthesizing a variety of stable and metastable
alloy phases [13]. Some of the important parameters that have an
effect on the final constitution of the powder are the milling speed,
milling time and ball-to-powder weight ratio. The milling time is
an important parameter and normally it is chosen to achieve a
steady state between the fracturing and cold welding of the powder
particles. The samples obtained from mechanical alloying are poly-
crystalline with aggregates of crystallites forming grains with grain
boundaries. The structure of the powders influences all its optoelec-
tronic and optical properties. As an example, the photoconductivity
response in polycrystalline materials composed of several micro-
crystallites has an additional adsorption band beyond the band
edge. This band is related with the decrease in crystalline size [6].
Different systems have been obtained by mechanochemical
synthesis reactions. Experiments reported by Suryanarayana [12]
shows successfully achieved reactions on binary and ternary com-
pounds related with copper and aluminum (CuO, CuO + Al) using
2 h milling time. Taking this into consideration, we decided to use
milling times equal or higher than 2 h. The prepared CdS nanopar-
ticle powder can be deposited in films by spraying, curtain coating,
roll coating, doctor blading, or screen-printing [13] for applications
in low-cost thin-film solar cells or thin photoconductive layers.
Although there are some reports on Cu doped CdS [3,11,14], so
far to our knowledge this is the first attempt to make Cu doped
CdS through mechanochemical alloying. Hence this paper focuses
on the preparation and structural characterization of Cu doped
CdS nanoparticles obtained by a simple mechanochemical route
0921-5107/$ – see front matter © 2012 Elsevier B.V. All rights reserved.
doi:10.1016/j.mseb.2012.03.002