ISSN 10274510, Journal of Surface Investigation. Xray, Synchrotron and Neutron Techniques, 2013, Vol. 7, No. 6, pp. 1270–1276. © Pleiades Publishing, Ltd., 2013.
1270
INTRODUCTION
Cadmium sulfide with a band gap of 2.42 eV is
employed as optical windows in creating heteroge
neous thinfilm photocells based on CdTe and
Cu(In, Ga)Se
2
[1]. In practice, when CdS nanoparti
cles grow along the normal to a transparent substrate
surface, it is possible to ensure the excellent properties
of solar cells and luminescent diodes due to efficient
charge transfer to electrodes. Solar cells with a set of
ordered cadmium sulfide particles are characterized
by a large area of the donor–acceptor interface and the
minimum charge transfer length, which offer their
advantage over bilayer structures [2]. Cadmium sulfide
nanoparticle growth has been investigated compre
hensively by means of different methods in [3–12]. In
this work, the surface morphologies of cadmium sul
fide films created via the electrochemical and chemi
cal deposition methods are compared to reveal their
features.
EXPERIMENTAL
Thin cadmium sulfide films were prepared by
means of electrochemical or chemical deposition
from different electrolytes onto glass coated with a
conducting SnO
2
+ In
2
O
3
film known as indiumtin
oxide (ITO) film. This layer has a sufficiently low elec
tric resistance (15 Ω/cm). After deposition, films were
annealed in air at T = 400°C for 20 min. The film
thickness was 500 ± 50 nm. Electrodeposition was per
formed from aqueous electrolytic solutions with the
help of the technique described in [7]. A chemical
deposition process was implemented by means of the
technique [9–11] having two variants:
(i) Single chemical deposition from a solution on
transparent conducting glass/ITO substrates [9, 10].
(ii) Successive deposition of several layers on pure
glass by submersion into a chemical bath [11].
The surface morphology of CdS films was studied
via atomicforce microscopy (AFM) in a JSPM5200
microscope under semicontact conditions with the use
of an NSC 35/AIBS cantilever with a curvature radius
of ≤10 nm. Scanning was carried out at atmospheric
pressure and room temperature.
Investigations were partially performed using an
NT–MDT atomicforce microscope and a Quanta
3D 200 scanning electron microscope (with crosssec
tion imaging). The film transmission spectra were
measured at wavelengths 0.19–3.00 μm with the help
of a Varian Cary500 Scan spectrophotometer (United
States) and an UV1 Helios Alpha instrument. The
film absorption edge was estimated from absorption
spectra. For this purpose, the multiple layerbylayer
growth of CdS films was carried out to select the
resulting thickness of coatings at which their optical
density D = αh (in the absorption edge region) was in
the range of 0.1–0.8 (i.e., from 80 to 17% of transmis
sion), being optimal for decreasing the relative error of
the determination of the optical density and absorp
tion coefficient.
RESULTS AND DISCUSSION
Surface Morphology
Electrodeposited thin CdS films were synthesized
using an electrolyte containing 0.30 M CdCl
2
and
0.03 M (Na)
2
S
2
O
3
on glass coated with a conducting
ITO film [7]. The film thickness was 500 ± 50 nm.
Electron Microscopic Study of Thin CdS Films
M. B. Dergacheva
a
, K. A. Mit’
b
, K. A. Urazov
c
, and V. F. Gremenok
d
a
Sokolsky Institute of Organic Catalysis and Electrochemistry, Almaty, Kazakhstan
b
Physicotechnical Institute, Almaty, Kazakhstan
c
KazakhBritish Technical University, Almaty, Kazakhstan
d
Scientific and Practical Materials Research Center, National Academy of Sciences of Belarus, Minsk, Belarus
Received April 17, 2013
Abstract—The results obtained by investigating the surface morphology and optical properties of thin CdS
films formed on transparent glass and glass/indiumtin oxide (ITO) substrates via the chemical and electro
chemical methods are presented. Thin cadmium sulfide films are employed as optical windows in thinfilm
polycrystalline solar cells. Closely packed cadmium sulfide nanoparticles are observed on the conducting
oxide (ITO) surface by means of atomicforce microscopy. Large particles (150–300 nm) comprise smaller
particles with sizes of 20–30 nm. Thin CdS layers are characterized by a relatively high level of transmission
(~60%) in the longwavelength spectral region (520–600 nm).
DOI: 10.1134/S1027451013130053