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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056
Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 686
Compositional, structural and optical properties analysis of β-In2S3
Thin Films Prepared by Chemical Spray Pyrolysis and Electrochemical
Deposition Techniques
D. Soro1,2, B. Fofana1,M. Sidibé3, B. Aka4, B. Mari2, S.Touré3
1Ecole Normale Superieure (ENS) d’Abidjan, 08 BP 10 Abidjan 08, Côte d’Ivoire
2Universitat Politècnica de Vàlencia, Departament de Física Aplicada-IDF, Camí de Vera s/n, Vàlencia, 46022,
Spain
3 Université FHB D’Abidjan-Cocody, Laboratoire d’Energie Solaire, 22 BP 582 Abidjan 22, Côte d’Ivoire
4 Université Nangui Abrogoua, UFR-SFA, 02 BP 801 Abidjan, Côte d’Ivoire
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract – An increased attention is devoted to interfacial
In2S3 thin films because of their potential application as anew
generation of buffer layer in copper indium galliumdiselenide
(CIGS)-based solar cells. In this paper, thin films of β-In2S3
were deposited by Chemical Spray Pyrolysis and
Electrochemical deposition onto FTO Coated GlassSubstrates.
Characterization of the films was carried out by X-ray
diffraction (XRD), Scanning Electron Microscopy (SEM),
Energy Dispersive Spectroscopy (EDS). Optical analysis to
determine band gap gives band gap varying from 2.45eV to
2.90 eV which are very close to the accepted values. The
structural analysis reveals films with (0 0 12) asmainpeak for
all samples in all case.
Key words : Indium sulfide, Buffer Layer,
electrodeposition ,Spray Pyrolysis, DMSO,FTO.
1.INTRODUCTION
Needless to say one of the crucial issues in recent decades
has been the increasing energy needs. When facing, as we
are to this problem, a transition out of the fossil civilization
is necessary. A promissing alternativesourceof energyisthe
use of solar cells. Finding viable alternatives also to silicon-
based photovoltaics, through low-cost solution processable
materials, is important. The international scientific
community constantlyfostersthedevelopmentofinnovative
solar energy transducing devices. In the recent decade a
large number of semiconductor materials havebeenstudied
for using in solar cells . Most promising materials for the use
as light absorbers in thin film solar cells are chalcopyrites
type semiconductors such as CIGS. CIGS absorbers need a
buffer layer to form photovoltaic heterojunctions.Currently
one of the best buffer materials for this purpose is a thin CdS
film [1]. However, the use of cadmium in PV devices is
undesirable from the view point of environmental safety [2].
Serious efforts have been made to substitute the CdS buffer
layer by other non-toxic low-absorbing materials. Indium
sulfide (In2S3) thin films as an n-type semiconductor have
recently attracted considerable attention because of their
interesting physical properties, which are suitable for
optoelectronic device fabrication. These films have a great
potential for photovoltaic applications .In2S3 is one of the
possible candidates to replace CdS as buffer layer. This
compound can be foundunderthreepolymorphicforms. The
cubic α uform [3] is stable above 693 K and crystallizes in
the defect spine! structure (a = 10.77Ȧ). The stable room
temperature phase is β-In2S3 [4]. A third modification (γ-
In2S3) with trigonal symmetryhasbeen reportedabove1047
K [5]. Depending upon the type and composition, the band
gap reported for In2S3 compound varies between 2.0 and
2.45 eV [6]. Hetero-junctures as CIGS/ β -In2S3 [7] or
CIS/In(OH,S) [8] have been built by CBD with conversion
efficiencies of 15.7% and 11.4% respectively. Indiumsulfide
has elaboratedusingvarious techniqueslikeSuccessiveIonic
Layer Adsorption and Reaction (SILAR) [9], Thermal
Evaporation (TE) [10], Atomic Layer Deposition (ADL) [11],
Chemical Bath Deposition (CBD) [12] etc. It was noted that
the quality of films depends strongly on growth technique.
Electrodeposition and Chemical Spray Pyrolysis are also
interesting for In2S3 synthesis. In the present work, we
prepared β-In2S3 by two different ways :Chemical Spray
Pyrolysis and Electrochemical deposition. The structure,
morphology,optical properties and composition were
studied and compared.
2. Experimental procedure
2.1. Preparation of thin films
Thin films of β-In2S3 were prepared by Chemical Spray
Pyrolysis and Electrochemical deposition onto FTO Coated
Glass Substrates.
Using Chemical Spray Pyrolysis, Indium sulfide (In2S3) thin
films were prepared onto FTO (Fluorine Doped Tin Oxide)
coated glass substrate from aqueous solution containing
indium (III) chloride (InCl3) (99.999%), thiourea (CS(NH2)2)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056
Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 687
(≥99%) and alcohol (5% in volume) to reduce the surface
tension. The concentration of indium chloride was fixed at
0.026M and the [S]/[In] ratio was 3. The substrate
temperature varied 250°C-277°C-300°C-330°C. The volume
sprayed was 5mL, the spray rate 1.5mL/min, the air
compressed pressure 0.7 bar and the distance between the
glass substrateand nozzle was kept to 30 cm. Glasssubstrate
were previously washed with HNO3andsubsequentlyrinsed
with water, ethanol and acetone.
Using electrodeposition, the In2S3 films were deposited by
pulsedpotentiostaticelectrodepositionfromaDMSOsolution
composed of 50 mM of sulfur (S8, Merck 99.8%), 40 mM
indium perchlorate (In(ClO4)3, Aldrich 98%) and 10 mM
potassium perchlorate (KClO4, Aldrich >99%) as supporting
electrolyte. The temperature of the electrolytic bath was
70°C. The working electrode substrates were glass plates
coated with FTO (SnO2:F). The electrodes were rinsed and
subsequently cleaned in an ultrasonic bath with acetone and
chemically treated in fresh 1M nitricacid solution for20min
at room temperature to improve the adherence of the films.
Then, they were carefully rinsed with distilled water and
dried with a nitrogen stream. The electrodeposition
potentials were performed applying a pulsed E/t program
using a three-electrode conventional arrangement. The
counter electrode was a platinum wire (99.99%) and a
Ag/AgCl sat. (E° = +0.199 V vs. NHE) was used as reference
electrode, all the potentials reported in this workrefertothis
electrode. Electrochemical measurements were performed
using an Ecochimie Potentiostat/Galvanostat, Autolab
PGSTAT100 model.
2.2. Preparation of thin films
The surface morphology and microanalysis using Energy
Dispersive X-ray Spectroscopy (EDS) of all the films were
obtained on a Jeol-JSM6300. Structural properties were
characterizedbymeansX-raydiffraction(XRD)measurement
with a Rigaku Ultima IV diffractometer using a parallel beam
in grazing incidence. In this configuration the angle of the
incident beam remains constant (ɵi) while thedetectorangle
moves 2ɵ. The parallel beamwas obtained bypassingtheCu-
Kα radiation of an X-ray tube through a CBO module. The
samples were scanned from 2ɵ = 15 to 60ºinstepsof0.02ºat
a speed of 1º/min. Optical properties were monitored by
transmittance using a Xe lamp in association with a 550 mm
Yvon–Jobin Triax-550 spectrophotometer using a back-
thinned CCD detector (Hammamatsu) optimized for the UV–
VIS range.
3. Results and discussion
3.1 Structural properties
The Thin films Structural of β -In2S3 properties prepared by
Chemical Spray Pyrolysis were characterizedbymeansX-ray
diffraction (XRD) measurement with a Rigaku Ultima IV
diffractometer in the ɵ-2ɵ configuration and using CuKα
radiation (1.5418Å). Figure 1 shows the XRD patternsofthin
films β -In2S3 prepared by Chemical Spray Pyrolysis at
different substrate temperatures. All films deposited are
polycrystalline with (0 0 12) as preferential direction
perpendicular to substrate plan. others peaks appeared at
14.17°- 22.30°- 23.48°- 27.54°- 43.96° and 48.06°
corresponding to (103), (107), (116), (109), (1 015)and(22
12).
10 20 30 40 50 60
XRDIntensity/a,u,
2(degree)
# #
#
(103)
(109)
(2212)
#
(0012)
# FTO
(1015)
250°C
277°C
300°C
330°C
Fig-1: X-ray diffraction spectra for films deposited by
Chemical Spray Pyrolysis at different FTO coated glass
substrate temperatures
Fig- 2 shows the XRD pattern of a In2S3 thin film formed by
electrochemical deposition at -1.125 V and recorded at
grazing incidence for two different incident angles (ɵi =0.4
and 0.5º). indeed, grazing incidence measurements are
performed at very low incident angles to maximizethesignal
from the thin layers. This is important when it is desired to
attenuate the influence of the substrate. Dots correspond to
FTO substrateReferencepatternJCPDS#25-0390relatestoa
tetragonal structure. In this reference only XRD peaks with
intensity higher than 15% have been plotted. All films
deposited are also polycrystalline with (0 0 12) as
preferential direction. The intensity of XRD peaks
corresponding to FTO substrate (labelled with dots)
decreases when the incident angle changes from 0.5 to 0.4º
while the signal coming from the top layer remains constant.
Some Peaks (103 ) and (109) are appeared only in films
deposited by Spray Pyrolysis with high intensity and other
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056
Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 688
(118) (116) (419) appeared on those deposited by
Electrodeposition . Comparing the X-ray diffraction spectra
(Fig-1 and Fig-2),wenoticethatalthoughtheoverallmajority
crystalstructureappears identical. The mean crystallitesize,
D, has been determined from line width of the XRD patterns
by using the Scherrer equation [15]:
D =
where K is a constant close to 1 (K = 0.9 was used), λx is theX-
ray wavelength whose value is 1.54Å (CuKα), β is the full
width at half maximum(FWHM) of the peak corrected bythe
instrumental broadening, while θ is the Bragg angle at the
center of the peak. The crystallite size D obtained from this
equation corresponds to the mean minimum dimension of a
coherent diffraction domain. When determining the
crystallite sizes, the (0 0 12) diffraction peak has been used,
because is the strongest one in all the samples, what leads to
less uncertainty in broadening determination. According to
this procedure, a crystallite size of about 25 nm has been
roughlycalculated forIn2S3 filmsbyElectrodepositionand35
nm for those deposited by Chemical Spray Pyrolysis .
20 30 40 50 60
(1,1,8)
(4,1,9)


(1,0,15)



(2,2,12)
(0,0,12)
XRDIntensity/a.u.
2 / degree
Incident angle= 0.5 deg
Incident angle= 0.4 deg
(1,1,6)
Fig-2: XRD pattern of electrodeposited In2S3 layers at -
1.125V recorded under grazing incidence.
3.2. Surface morphology
Scanning Electron Microscopy (SEM) is a convenientmethod
to study microstructure of thin films. It was utilized to study
the surface morphologyofindiumsulfidethinfilmsdeposited
by Chemical Spray Pyrolysis and Electrochemical deposition
onto FTO Coated Glass Substrates. Films deposited by
Chemical Spray Pyrolysis were well-covered, homogeneous,
dense, continuous and compact with no cracks neithervoids.
Grains are very small (Fig- 3).The small grain size results
from the quick cristallisation betwtween the precursors
during the film drying. Otherwise grainssizeisbigexplaining
by agglomeration of small grains to form big one. Debye
Scherrer’s formula derived to XRD confirms well those
results.
Fig-3: SEM micrographs of In2S3 thin films at different
substrates temperatures
Fig- 4 shows typical SEM surface morphologies for three
different In2S3 thinfilmselectrochemicallyobtainedontoFTO
substrates in a potential interval comprised between –1.125
V and –1.175 V. The images showauniformmorphologywith
crystallites of very small size which agrees with the analysis
of grazing XRD patterns. Themorphologiccharacteristicsare
independent of theelectrochemicalpotentialemployedinthe
synthesis. the predominant phases are In2S3 (tetragonal
spinel β-In2S3). In fact, the morphological characteristic
observed are entirelyconsistentwiththoseobtainedforIn2S3
thin films formed in aqueous solution through of chemical
bath deposition (CBD) [13,14]. Thus, all the samples show a
cauliflower like morphology with aggregates .
In conclusion , all the films obtained by the two different
ways show good uniformity and adherence.
Fig-4: SEM micrographs for three typical In2S3 thin films
electrochemicallygrownontoFTOsubstratesat:(a)–1.125V,
(b) –1.150 V and (c) –1.175 V respectively
JCPDS #25-0390
FTO
FTO
a b c
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056
Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 689
3.3 Compositional Analysis
Energy Dispersive Spectroscopy (EDS) is a quantitative and
qualitative tool to measureatomic concentrationofelements
present in sample after elaboration. Atomic concentration of
In and S of samples obtained from EDS attached to SEM are
given in Table -1 and Table -2. We notice that all samples
elaborated have good stoichiometry.
Table -1: Composition of In2S3 /FTO glass substrate
obtained EDS at different temperatures
Ts (ºC) at% S at% In Experimental Atomic Ratio S/In
250°C 59.69 40.31 1.48
277°C 59.00 41.00 1.43
300°C 57.55 42.45 1.35
330°C 54.25 45.75 1.18
Table -2: Composition ofIn2S3/FTOglasssubstrateobtained
EDS for three different In2S3 thin films electrochemically
grown at different electrodeposition potential.
The EDAX analysis of In2S3 thin films electrochemically
grown onto FTO substrates shows an appropriate
composition with an atomic ratioveryclosetothetheoretical
values (see Table -2). The decreasing in the atomic ratio at
more cathodic potential indicates that the films present a
small indium excess.
We noted that all samples either elaborated by Chemical
Spray Pyrolysis or Electrochemical deposition have good
stoichiometry.
3.4. Optical properties
Optical studies of In2S3 films were carried out in the visible
range using a spectrophotometer HR-4000 OceanOpticsThe
transmittance T versus ʎ spectrum of films deposited by
Chemical Spray Pyrolysis and Electrochemical deposition
show that films have better transmittance .Allthefilmsshow
more than 55 % transmission for wavelengths longer than
500 nm (Fig- 5 and Fig- 7). The sharp rise in transmission
near 500 nm is an identification of good crystallinity of
films.Optical absorption spectra recorded in the wavelength
region 250-1000nm in order to determine the optical band
gap, graph was plotted with (αhν)2 against hν. Optical band
gap was determined from this plot for all films by linear fit in
the straight portion of the graph.Forthethinfilmobtainedby
Electrochemical deposition , the band gap energy values
decreasing from 2.80 eV to 2.45 eV(Fig- 8)after the heat
treatment which is very close to the accepted value [16].
Films prepared Spray Pyrolysis have band gap larger (from
2.73 eV to 2.90 eV) (Fig- 6). The change in thebandgapvalue
can be correlated with possible nano-crystal sizes through
the nano-crystal size effects, whichagreeswiththecrystallite
size found through the grazing XRD analysis.
300 400 500 600 700 800 900 1000
0
10
20
30
40
50
60
70
80
90
100
FTO
300°C
330°C
250°C
277°C
Transmittance(%)
(nm)
Fig-5: Transmittance spectra of samples at different
substrates temperatures
Ed/V (120s) %at In %at S
Experimental Atomic Ratio
S/In
Theoretic
values
40 60 1.50
-1.25 38.56 61.44 1.59
-1.50 39.21 60.78 1.55
-1.75
39.80 60.20 1.51
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056
Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 690
2,0 2,5 3,0 3,5
0
2
4
6
8
10
250°C-Eg=2,73eV
277°C-Eg=2,82eV
300°C-Eg=2,86eV
330°C-Eg=2,90eV
(AE)
2
h(eV)
Fig-6: Band gap variation of samples at different
substrates temperature
250 500 750 1000
0
20
40
60
80
100
Transmittance/%
 / nm
(a)
Fig-7:Transmittance of a In2S3 thin film electrochemically
formed onto FTO substrate at-1.125 V, the figure show the
spectral response (a) as grown and (b) after a heattreatment
at 450°C for 30 min, the (c) represent the optical response of
FTO substrate.
1,5 2,0 2,5 3,0 3,5
0,0
0,5
1,0
1,5
(b)
(h)
2
/eV
2
m
-2
x10
14
h / eV
Fig-7:Determination of bandgap energy through the (αhν)2
vs hν plot for the same sample ( ) before and ( ) after heat
treatment.
4. CONCLUSIONS
β-In2S3 thin films were fabricated by using two different
ways :Chemical Spray Pyrolysis and Electrochemical
deposition.Films grown by Electrochemical deposition have
lower crystallinity than those grown by Chemical Spray
Pyrolysis .All thin films show a similar X-ray diffraction
pattern. Indeed, X-ray diffraction analysis reveal that all thin
films are polycrystalline with (0 0 12) as main peak which
has high intensity . XRD peaks located at 2ɵ angles of 27.47,
33.23, 43.60, and 47.70 are also clearly identified and match
well with the JCPDS #25-0390 pattern corresponding to a
tetragonal phase of In2S3. SEM images revealed good
substrate coverage and microstructure whereas EDAX
analysis gave a stoichiometric composition very close to the
expected. Optical measurements allowed to establish the
band gap of In2S3 . The results reveal that the microstructure
and the optical properties of the In2S3 films are highly
dependent on the growth method. Films prepared Spray
Pyrolysis have band gap larger (from 2.73 eV to 2.90 eV) and
the band gap energy values decreasing from 2.80 eV to 2.45
eV(Fig- 8) after the heat treatment forthe thin film obtained
by Electrochemical. In all cases ,gap energy values of all the
thin films ranges from 2.45 eV to 2.90 eV. This makes the
films suitable foroptoelectronicdevices,forinstancewindow
layers in solar cells.
REFERENCES
[1] W. Fuhs and R. Klenk, Thin-film solar cells-overview,
Proc. 2nd World Conf. and Exhibition on Photovoltaic Solar
Energy Conv., 6–10 (1998) p 381, Vienna.
[2].K.M. Hynes, J. Newham, Proceedings 16th European
Photovoltaic Solar Energy Conference, (2000) p 2297.
[3 ] H. Hahn and W. Klinger Z., Inorg. Chem., Vol 260, (1949)
p 97.
[4] C. J. X. Rooymans J Inorg. Nucl. Chem., Vol 260, (1959)
p78.
[5] J. V. Landuyt, H. HatwelI and S. AmeIinekx Mater. Res.
Bull., Vol 3 , (I 968) p 59.
[6]D. Hariskos, M. Ruckh, U. Rühle, T. Walter, H. W. Schock, J.
Hedström and L. Stolt, Sol. Energy Mater. Sol. Cells, Vol 41,
(1996) p 345.
[7] D. Braunger, D. Hariskos, T. Walter, H.W. Shock, Material
Solar Cells, Vol 40 ,(1997), p 97.
[8] Kuveshni Govender, David S. Boyle and Paul O’Brien, J.
Mater. Chem., Vol 13, (2003) p 2242.
[9]T. Sall, A. Raidou, S. Elfarrass, B. Hartiti, B. Mari, A.
Qachaou and M. Fahoume. Vol 46, (2014)P 247.
c
a
b
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056
Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 691
[10] A. A. EL Shazly, D. Abdelkady, H.S. Metoually, M.A.M.
Segmam, .thin films.Vol 10, (March1998) p 5943.
[11] T. Asikainen, M. Ritala, and M. Leskelä,“GrowthofIn2S3
thin films by atomic layer epitaxy,” Applied Surface Science,
Vol 82-83, (December 1994) p 122 .
[12] T. Dedova, J. Wienke, M. Goris, M. Krunks, Thin Solid
Films, Vol 515, (May 2007), p 6064.
[13] W. Vallejo, J. Clavijo, Brazilian Journal ofPhysics,Vol 40 ,
(2010) p 30.
[14]P. O’Brien, D. J. Otway, and J. R.Walsh, Thin Solid Films,
Vol 315, (1998) p 57.
BIOGRAPHY
Dr. D. Soro is the corresponding
author of this paper and a post
graduate Université Nangui
Abrogoua, UFR-SFA, 02 BP 801
Abidjan, Côte d’Ivoire. He is a
Professor at (ENS) Abidjan, Côte
d’Ivoire 08 BP 10 Abidjan 08.
mail: donafologosoro@yahoo.fr
Dr B. Fofana, (ENS)Abidjan, Côte
d’Ivoire 08 BP 10 Abidjan 08,
Laboratory IREN, Université
Nangui Abrogoua, UFR-SFACôte
d’Ivoire.
Dr M.Sidibé,Université FHB
D’Abidjan-Cocody, 22 BP 582
Abidjan 22, Côte d’Ivoire
Laboratory of Solar Energy.
Aka Boko , professor, Université
Nangui Abrogoua, UFR-SFA, 02
BP 801 Abidjan, Côte d’Ivoire,
Laboratory IREN UFR-SFA
Côte d’Ivoire.
.
Bernabé Marí
Soucase ,professor, Universitat
Politècnica de València, Valencia
Departament de Física Aplicada-
IDF, Camí de Vera s/n, Vàlencia,
46022, Spain.
S.Touré,UniversitéFHB
D’Abidjan-Cocody, Laboratory of
Solar Energy, 22 BP 582 Abidjan
22, Côte d’Ivoire.

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Compositional, structural and optical properties analysis of β-In2S3 Thin Films Prepared by Chemical Spray Pyrolysis and Electrochemical Deposition Techniques

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 686 Compositional, structural and optical properties analysis of β-In2S3 Thin Films Prepared by Chemical Spray Pyrolysis and Electrochemical Deposition Techniques D. Soro1,2, B. Fofana1,M. Sidibé3, B. Aka4, B. Mari2, S.Touré3 1Ecole Normale Superieure (ENS) d’Abidjan, 08 BP 10 Abidjan 08, Côte d’Ivoire 2Universitat Politècnica de Vàlencia, Departament de Física Aplicada-IDF, Camí de Vera s/n, Vàlencia, 46022, Spain 3 Université FHB D’Abidjan-Cocody, Laboratoire d’Energie Solaire, 22 BP 582 Abidjan 22, Côte d’Ivoire 4 Université Nangui Abrogoua, UFR-SFA, 02 BP 801 Abidjan, Côte d’Ivoire ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract – An increased attention is devoted to interfacial In2S3 thin films because of their potential application as anew generation of buffer layer in copper indium galliumdiselenide (CIGS)-based solar cells. In this paper, thin films of β-In2S3 were deposited by Chemical Spray Pyrolysis and Electrochemical deposition onto FTO Coated GlassSubstrates. Characterization of the films was carried out by X-ray diffraction (XRD), Scanning Electron Microscopy (SEM), Energy Dispersive Spectroscopy (EDS). Optical analysis to determine band gap gives band gap varying from 2.45eV to 2.90 eV which are very close to the accepted values. The structural analysis reveals films with (0 0 12) asmainpeak for all samples in all case. Key words : Indium sulfide, Buffer Layer, electrodeposition ,Spray Pyrolysis, DMSO,FTO. 1.INTRODUCTION Needless to say one of the crucial issues in recent decades has been the increasing energy needs. When facing, as we are to this problem, a transition out of the fossil civilization is necessary. A promissing alternativesourceof energyisthe use of solar cells. Finding viable alternatives also to silicon- based photovoltaics, through low-cost solution processable materials, is important. The international scientific community constantlyfostersthedevelopmentofinnovative solar energy transducing devices. In the recent decade a large number of semiconductor materials havebeenstudied for using in solar cells . Most promising materials for the use as light absorbers in thin film solar cells are chalcopyrites type semiconductors such as CIGS. CIGS absorbers need a buffer layer to form photovoltaic heterojunctions.Currently one of the best buffer materials for this purpose is a thin CdS film [1]. However, the use of cadmium in PV devices is undesirable from the view point of environmental safety [2]. Serious efforts have been made to substitute the CdS buffer layer by other non-toxic low-absorbing materials. Indium sulfide (In2S3) thin films as an n-type semiconductor have recently attracted considerable attention because of their interesting physical properties, which are suitable for optoelectronic device fabrication. These films have a great potential for photovoltaic applications .In2S3 is one of the possible candidates to replace CdS as buffer layer. This compound can be foundunderthreepolymorphicforms. The cubic α uform [3] is stable above 693 K and crystallizes in the defect spine! structure (a = 10.77Ȧ). The stable room temperature phase is β-In2S3 [4]. A third modification (γ- In2S3) with trigonal symmetryhasbeen reportedabove1047 K [5]. Depending upon the type and composition, the band gap reported for In2S3 compound varies between 2.0 and 2.45 eV [6]. Hetero-junctures as CIGS/ β -In2S3 [7] or CIS/In(OH,S) [8] have been built by CBD with conversion efficiencies of 15.7% and 11.4% respectively. Indiumsulfide has elaboratedusingvarious techniqueslikeSuccessiveIonic Layer Adsorption and Reaction (SILAR) [9], Thermal Evaporation (TE) [10], Atomic Layer Deposition (ADL) [11], Chemical Bath Deposition (CBD) [12] etc. It was noted that the quality of films depends strongly on growth technique. Electrodeposition and Chemical Spray Pyrolysis are also interesting for In2S3 synthesis. In the present work, we prepared β-In2S3 by two different ways :Chemical Spray Pyrolysis and Electrochemical deposition. The structure, morphology,optical properties and composition were studied and compared. 2. Experimental procedure 2.1. Preparation of thin films Thin films of β-In2S3 were prepared by Chemical Spray Pyrolysis and Electrochemical deposition onto FTO Coated Glass Substrates. Using Chemical Spray Pyrolysis, Indium sulfide (In2S3) thin films were prepared onto FTO (Fluorine Doped Tin Oxide) coated glass substrate from aqueous solution containing indium (III) chloride (InCl3) (99.999%), thiourea (CS(NH2)2)
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 687 (≥99%) and alcohol (5% in volume) to reduce the surface tension. The concentration of indium chloride was fixed at 0.026M and the [S]/[In] ratio was 3. The substrate temperature varied 250°C-277°C-300°C-330°C. The volume sprayed was 5mL, the spray rate 1.5mL/min, the air compressed pressure 0.7 bar and the distance between the glass substrateand nozzle was kept to 30 cm. Glasssubstrate were previously washed with HNO3andsubsequentlyrinsed with water, ethanol and acetone. Using electrodeposition, the In2S3 films were deposited by pulsedpotentiostaticelectrodepositionfromaDMSOsolution composed of 50 mM of sulfur (S8, Merck 99.8%), 40 mM indium perchlorate (In(ClO4)3, Aldrich 98%) and 10 mM potassium perchlorate (KClO4, Aldrich >99%) as supporting electrolyte. The temperature of the electrolytic bath was 70°C. The working electrode substrates were glass plates coated with FTO (SnO2:F). The electrodes were rinsed and subsequently cleaned in an ultrasonic bath with acetone and chemically treated in fresh 1M nitricacid solution for20min at room temperature to improve the adherence of the films. Then, they were carefully rinsed with distilled water and dried with a nitrogen stream. The electrodeposition potentials were performed applying a pulsed E/t program using a three-electrode conventional arrangement. The counter electrode was a platinum wire (99.99%) and a Ag/AgCl sat. (E° = +0.199 V vs. NHE) was used as reference electrode, all the potentials reported in this workrefertothis electrode. Electrochemical measurements were performed using an Ecochimie Potentiostat/Galvanostat, Autolab PGSTAT100 model. 2.2. Preparation of thin films The surface morphology and microanalysis using Energy Dispersive X-ray Spectroscopy (EDS) of all the films were obtained on a Jeol-JSM6300. Structural properties were characterizedbymeansX-raydiffraction(XRD)measurement with a Rigaku Ultima IV diffractometer using a parallel beam in grazing incidence. In this configuration the angle of the incident beam remains constant (ɵi) while thedetectorangle moves 2ɵ. The parallel beamwas obtained bypassingtheCu- Kα radiation of an X-ray tube through a CBO module. The samples were scanned from 2ɵ = 15 to 60ºinstepsof0.02ºat a speed of 1º/min. Optical properties were monitored by transmittance using a Xe lamp in association with a 550 mm Yvon–Jobin Triax-550 spectrophotometer using a back- thinned CCD detector (Hammamatsu) optimized for the UV– VIS range. 3. Results and discussion 3.1 Structural properties The Thin films Structural of β -In2S3 properties prepared by Chemical Spray Pyrolysis were characterizedbymeansX-ray diffraction (XRD) measurement with a Rigaku Ultima IV diffractometer in the ɵ-2ɵ configuration and using CuKα radiation (1.5418Å). Figure 1 shows the XRD patternsofthin films β -In2S3 prepared by Chemical Spray Pyrolysis at different substrate temperatures. All films deposited are polycrystalline with (0 0 12) as preferential direction perpendicular to substrate plan. others peaks appeared at 14.17°- 22.30°- 23.48°- 27.54°- 43.96° and 48.06° corresponding to (103), (107), (116), (109), (1 015)and(22 12). 10 20 30 40 50 60 XRDIntensity/a,u, 2(degree) # # # (103) (109) (2212) # (0012) # FTO (1015) 250°C 277°C 300°C 330°C Fig-1: X-ray diffraction spectra for films deposited by Chemical Spray Pyrolysis at different FTO coated glass substrate temperatures Fig- 2 shows the XRD pattern of a In2S3 thin film formed by electrochemical deposition at -1.125 V and recorded at grazing incidence for two different incident angles (ɵi =0.4 and 0.5º). indeed, grazing incidence measurements are performed at very low incident angles to maximizethesignal from the thin layers. This is important when it is desired to attenuate the influence of the substrate. Dots correspond to FTO substrateReferencepatternJCPDS#25-0390relatestoa tetragonal structure. In this reference only XRD peaks with intensity higher than 15% have been plotted. All films deposited are also polycrystalline with (0 0 12) as preferential direction. The intensity of XRD peaks corresponding to FTO substrate (labelled with dots) decreases when the incident angle changes from 0.5 to 0.4º while the signal coming from the top layer remains constant. Some Peaks (103 ) and (109) are appeared only in films deposited by Spray Pyrolysis with high intensity and other
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 688 (118) (116) (419) appeared on those deposited by Electrodeposition . Comparing the X-ray diffraction spectra (Fig-1 and Fig-2),wenoticethatalthoughtheoverallmajority crystalstructureappears identical. The mean crystallitesize, D, has been determined from line width of the XRD patterns by using the Scherrer equation [15]: D = where K is a constant close to 1 (K = 0.9 was used), λx is theX- ray wavelength whose value is 1.54Å (CuKα), β is the full width at half maximum(FWHM) of the peak corrected bythe instrumental broadening, while θ is the Bragg angle at the center of the peak. The crystallite size D obtained from this equation corresponds to the mean minimum dimension of a coherent diffraction domain. When determining the crystallite sizes, the (0 0 12) diffraction peak has been used, because is the strongest one in all the samples, what leads to less uncertainty in broadening determination. According to this procedure, a crystallite size of about 25 nm has been roughlycalculated forIn2S3 filmsbyElectrodepositionand35 nm for those deposited by Chemical Spray Pyrolysis . 20 30 40 50 60 (1,1,8) (4,1,9)   (1,0,15)    (2,2,12) (0,0,12) XRDIntensity/a.u. 2 / degree Incident angle= 0.5 deg Incident angle= 0.4 deg (1,1,6) Fig-2: XRD pattern of electrodeposited In2S3 layers at - 1.125V recorded under grazing incidence. 3.2. Surface morphology Scanning Electron Microscopy (SEM) is a convenientmethod to study microstructure of thin films. It was utilized to study the surface morphologyofindiumsulfidethinfilmsdeposited by Chemical Spray Pyrolysis and Electrochemical deposition onto FTO Coated Glass Substrates. Films deposited by Chemical Spray Pyrolysis were well-covered, homogeneous, dense, continuous and compact with no cracks neithervoids. Grains are very small (Fig- 3).The small grain size results from the quick cristallisation betwtween the precursors during the film drying. Otherwise grainssizeisbigexplaining by agglomeration of small grains to form big one. Debye Scherrer’s formula derived to XRD confirms well those results. Fig-3: SEM micrographs of In2S3 thin films at different substrates temperatures Fig- 4 shows typical SEM surface morphologies for three different In2S3 thinfilmselectrochemicallyobtainedontoFTO substrates in a potential interval comprised between –1.125 V and –1.175 V. The images showauniformmorphologywith crystallites of very small size which agrees with the analysis of grazing XRD patterns. Themorphologiccharacteristicsare independent of theelectrochemicalpotentialemployedinthe synthesis. the predominant phases are In2S3 (tetragonal spinel β-In2S3). In fact, the morphological characteristic observed are entirelyconsistentwiththoseobtainedforIn2S3 thin films formed in aqueous solution through of chemical bath deposition (CBD) [13,14]. Thus, all the samples show a cauliflower like morphology with aggregates . In conclusion , all the films obtained by the two different ways show good uniformity and adherence. Fig-4: SEM micrographs for three typical In2S3 thin films electrochemicallygrownontoFTOsubstratesat:(a)–1.125V, (b) –1.150 V and (c) –1.175 V respectively JCPDS #25-0390 FTO FTO a b c
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 689 3.3 Compositional Analysis Energy Dispersive Spectroscopy (EDS) is a quantitative and qualitative tool to measureatomic concentrationofelements present in sample after elaboration. Atomic concentration of In and S of samples obtained from EDS attached to SEM are given in Table -1 and Table -2. We notice that all samples elaborated have good stoichiometry. Table -1: Composition of In2S3 /FTO glass substrate obtained EDS at different temperatures Ts (ºC) at% S at% In Experimental Atomic Ratio S/In 250°C 59.69 40.31 1.48 277°C 59.00 41.00 1.43 300°C 57.55 42.45 1.35 330°C 54.25 45.75 1.18 Table -2: Composition ofIn2S3/FTOglasssubstrateobtained EDS for three different In2S3 thin films electrochemically grown at different electrodeposition potential. The EDAX analysis of In2S3 thin films electrochemically grown onto FTO substrates shows an appropriate composition with an atomic ratioveryclosetothetheoretical values (see Table -2). The decreasing in the atomic ratio at more cathodic potential indicates that the films present a small indium excess. We noted that all samples either elaborated by Chemical Spray Pyrolysis or Electrochemical deposition have good stoichiometry. 3.4. Optical properties Optical studies of In2S3 films were carried out in the visible range using a spectrophotometer HR-4000 OceanOpticsThe transmittance T versus ʎ spectrum of films deposited by Chemical Spray Pyrolysis and Electrochemical deposition show that films have better transmittance .Allthefilmsshow more than 55 % transmission for wavelengths longer than 500 nm (Fig- 5 and Fig- 7). The sharp rise in transmission near 500 nm is an identification of good crystallinity of films.Optical absorption spectra recorded in the wavelength region 250-1000nm in order to determine the optical band gap, graph was plotted with (αhν)2 against hν. Optical band gap was determined from this plot for all films by linear fit in the straight portion of the graph.Forthethinfilmobtainedby Electrochemical deposition , the band gap energy values decreasing from 2.80 eV to 2.45 eV(Fig- 8)after the heat treatment which is very close to the accepted value [16]. Films prepared Spray Pyrolysis have band gap larger (from 2.73 eV to 2.90 eV) (Fig- 6). The change in thebandgapvalue can be correlated with possible nano-crystal sizes through the nano-crystal size effects, whichagreeswiththecrystallite size found through the grazing XRD analysis. 300 400 500 600 700 800 900 1000 0 10 20 30 40 50 60 70 80 90 100 FTO 300°C 330°C 250°C 277°C Transmittance(%) (nm) Fig-5: Transmittance spectra of samples at different substrates temperatures Ed/V (120s) %at In %at S Experimental Atomic Ratio S/In Theoretic values 40 60 1.50 -1.25 38.56 61.44 1.59 -1.50 39.21 60.78 1.55 -1.75 39.80 60.20 1.51
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 690 2,0 2,5 3,0 3,5 0 2 4 6 8 10 250°C-Eg=2,73eV 277°C-Eg=2,82eV 300°C-Eg=2,86eV 330°C-Eg=2,90eV (AE) 2 h(eV) Fig-6: Band gap variation of samples at different substrates temperature 250 500 750 1000 0 20 40 60 80 100 Transmittance/%  / nm (a) Fig-7:Transmittance of a In2S3 thin film electrochemically formed onto FTO substrate at-1.125 V, the figure show the spectral response (a) as grown and (b) after a heattreatment at 450°C for 30 min, the (c) represent the optical response of FTO substrate. 1,5 2,0 2,5 3,0 3,5 0,0 0,5 1,0 1,5 (b) (h) 2 /eV 2 m -2 x10 14 h / eV Fig-7:Determination of bandgap energy through the (αhν)2 vs hν plot for the same sample ( ) before and ( ) after heat treatment. 4. CONCLUSIONS β-In2S3 thin films were fabricated by using two different ways :Chemical Spray Pyrolysis and Electrochemical deposition.Films grown by Electrochemical deposition have lower crystallinity than those grown by Chemical Spray Pyrolysis .All thin films show a similar X-ray diffraction pattern. Indeed, X-ray diffraction analysis reveal that all thin films are polycrystalline with (0 0 12) as main peak which has high intensity . XRD peaks located at 2ɵ angles of 27.47, 33.23, 43.60, and 47.70 are also clearly identified and match well with the JCPDS #25-0390 pattern corresponding to a tetragonal phase of In2S3. SEM images revealed good substrate coverage and microstructure whereas EDAX analysis gave a stoichiometric composition very close to the expected. Optical measurements allowed to establish the band gap of In2S3 . The results reveal that the microstructure and the optical properties of the In2S3 films are highly dependent on the growth method. Films prepared Spray Pyrolysis have band gap larger (from 2.73 eV to 2.90 eV) and the band gap energy values decreasing from 2.80 eV to 2.45 eV(Fig- 8) after the heat treatment forthe thin film obtained by Electrochemical. In all cases ,gap energy values of all the thin films ranges from 2.45 eV to 2.90 eV. This makes the films suitable foroptoelectronicdevices,forinstancewindow layers in solar cells. REFERENCES [1] W. Fuhs and R. Klenk, Thin-film solar cells-overview, Proc. 2nd World Conf. and Exhibition on Photovoltaic Solar Energy Conv., 6–10 (1998) p 381, Vienna. [2].K.M. Hynes, J. Newham, Proceedings 16th European Photovoltaic Solar Energy Conference, (2000) p 2297. [3 ] H. Hahn and W. Klinger Z., Inorg. Chem., Vol 260, (1949) p 97. [4] C. J. X. Rooymans J Inorg. Nucl. Chem., Vol 260, (1959) p78. [5] J. V. Landuyt, H. HatwelI and S. AmeIinekx Mater. Res. Bull., Vol 3 , (I 968) p 59. [6]D. Hariskos, M. Ruckh, U. Rühle, T. Walter, H. W. Schock, J. Hedström and L. Stolt, Sol. Energy Mater. Sol. Cells, Vol 41, (1996) p 345. [7] D. Braunger, D. Hariskos, T. Walter, H.W. Shock, Material Solar Cells, Vol 40 ,(1997), p 97. [8] Kuveshni Govender, David S. Boyle and Paul O’Brien, J. Mater. Chem., Vol 13, (2003) p 2242. [9]T. Sall, A. Raidou, S. Elfarrass, B. Hartiti, B. Mari, A. Qachaou and M. Fahoume. Vol 46, (2014)P 247. c a b
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 04 Issue: 01 | Jan -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 691 [10] A. A. EL Shazly, D. Abdelkady, H.S. Metoually, M.A.M. Segmam, .thin films.Vol 10, (March1998) p 5943. [11] T. Asikainen, M. Ritala, and M. Leskelä,“GrowthofIn2S3 thin films by atomic layer epitaxy,” Applied Surface Science, Vol 82-83, (December 1994) p 122 . [12] T. Dedova, J. Wienke, M. Goris, M. Krunks, Thin Solid Films, Vol 515, (May 2007), p 6064. [13] W. Vallejo, J. Clavijo, Brazilian Journal ofPhysics,Vol 40 , (2010) p 30. [14]P. O’Brien, D. J. Otway, and J. R.Walsh, Thin Solid Films, Vol 315, (1998) p 57. BIOGRAPHY Dr. D. Soro is the corresponding author of this paper and a post graduate Université Nangui Abrogoua, UFR-SFA, 02 BP 801 Abidjan, Côte d’Ivoire. He is a Professor at (ENS) Abidjan, Côte d’Ivoire 08 BP 10 Abidjan 08. mail: donafologosoro@yahoo.fr Dr B. Fofana, (ENS)Abidjan, Côte d’Ivoire 08 BP 10 Abidjan 08, Laboratory IREN, Université Nangui Abrogoua, UFR-SFACôte d’Ivoire. Dr M.Sidibé,Université FHB D’Abidjan-Cocody, 22 BP 582 Abidjan 22, Côte d’Ivoire Laboratory of Solar Energy. Aka Boko , professor, Université Nangui Abrogoua, UFR-SFA, 02 BP 801 Abidjan, Côte d’Ivoire, Laboratory IREN UFR-SFA Côte d’Ivoire. . Bernabé Marí Soucase ,professor, Universitat Politècnica de València, Valencia Departament de Física Aplicada- IDF, Camí de Vera s/n, Vàlencia, 46022, Spain. S.Touré,UniversitéFHB D’Abidjan-Cocody, Laboratory of Solar Energy, 22 BP 582 Abidjan 22, Côte d’Ivoire.