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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume 4 Issue 4, June 2020 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470
@ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1530
Preparation and Properties of
Nanocrystalline Zinc Oxide Thin Films
S. S. Kawar
Department of Physics, Shree Dr R G Rathod Arts and Science College, Murtajapur, Maharashtra, India
ABSTRACT
Metal oxide is highly important material whichpossesses manyuniqueoptical
and electrical properties for applications in manyareassuchasSolarcells,Gas
sensors and so on. With the developmentof researchand applicationsofMetal
oxide thin films, research results are verified that the morphology of Metal
oxide thin films are plays an important role in applications of these films.
Variety of morphologies, complex structurehasbeendevelopedbyphysical or
chemical methods. However the work on controlled growth of these films is
still in developing state. Therefore in present work we deposited ZnSandZnO
metal oxides thin films on different substrates by Chemical Bath Deposition
Technique. Structural, Surface Morphology and Optical properties of as
deposited films were investigated by XRD, SEM, and UV-VIS
Spectrophotometer. The band gap isalsocalculatedfromtheequation relating
absorption co-efficient to wavelength. The band gap indicates the film is
transmitting within the visible range and the band gaps changes because of
the grain size of the films. We also observed that, the change in preparative
parameters affects the deposition rate of thin films. From the observation,itis
clear that the growth rate increases as the deposition temperature, increases.
KEYWORDS: Metal Oxide Thin films, Nanostructure, Chemical bath Deposition
How to cite this paper: S. S. Kawar
"Preparation and Properties of
Nanocrystalline Zinc Oxide Thin Films"
Published in
International Journal
of Trend in Scientific
Research and
Development(ijtsrd),
ISSN: 2456-6470,
Volume-4 | Issue-4,
June 2020, pp.1530-
1533, URL:
www.ijtsrd.com/papers/ijtsrd31623.pdf
Copyright © 2020 by author(s) and
International Journal ofTrendinScientific
Research and Development Journal. This
is an Open Access article distributed
under the terms of
the Creative
CommonsAttribution
License (CC BY 4.0)
(http://creativecommons.org/licenses/by
/4.0)
INTRODUCTION:
Electronic semiconductor devices and Photovoltaic devices
are the main applications resultedinattremendous increase
of innovative thin film processing technology. For the
improvement of the technology, the materials of different
properties and qualities are needed. The synthesis and
characterization of various wide band gap metal oxide
nanostructures such as nanowires, nanorods, nanobelts,
nanobridges and nanowalls has attracted great interest due
to their size, morphology related properties, and their
emerging applications in novel functional nanodevices[1,2].
Recently, research and development of alternative energy
technologies, such as low cost flatpanel solar cells thin film
devices, and many otherinnovativeconceptshaveincreased.
Metal Oxides such as ZnO, TiO2 is an important
multifunctional material which has received great attention
during the last few years due to their unique applications in
microelectronic and optoelectronic devices, and for self-
assembled growth of three dimensional nano scale systems
[3, 4]. Metal oxide nano structures have the potential to
significantly improve the performance and durability of
certain devices used in areas of importance: energy
production and homeland security. A key challenge in this
research is to deposit nano structured metal oxide thinfilms
with consistent morphology and reproducible properties
with a long term stability.
Therefore in present work we deposited ZnO metal oxide
thin films on different substrates by Chemical Bath
Deposition Technique. A nanostructured thin film of Zinc
oxide (ZnO) have been obtained from Zinc sulphide (ZnS)
films by annealing process in air at temperatures between
400ºC and 750ºC. The ZnS films have been fabricated onto
glass substrates using simple & inexpensive chemical bath
deposition technique (CBDT). The optical & structural
characterization of obtained materials was performed. The
x-ray diffraction (XRD) study has confirmedtheformation of
ZnO with nano-size scale whereas the scanning electron
microscopy (SEM) studies showed that all the films were
polycrystalline in nature. Theoptical energybandgapsof the
films were evaluated. The nano-crystalline materials
exhibiting small particle size & large surface area may be
applied for various gas sensors as well as in large area
Optoelectronic devices.
MATERIAL AND METHODS:
To prepare ZnO films, aqueous solutions of zinc sources and
thiourea with calculated proportion was added in 130 ml of
de-ionized water. Complexing agent ammonia was added
slowly to adjust the pH of the solution. The solution was
stirred and transferred to another container containing
substrate. The resulting solution was kept at 70±2ºC for 1
hour. The substrate used is commercial glass slide. Cleaning
of substrate is important in fabrication of thinfilms,cleaning
steps and growth procedure is reported elsewhere [5-7].
After 20-30 minutes the bath solution in beaker turned
whitish, thus indicating the onsetZnSdepositionontheglass
slide. After a reaction time of 1 hour the glass slides were
taken out and dried in air for 15 minutes. Then for the post
annealing treatment in air, the prepared ZnSfilms werekept
IJTSRD31623
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1531
in the oven at various temperatures between 400ºC and
750ºC for 10 hours. The ZnS films get oxidized in the oven to
form thin films of ZnO.
The crystallographic structure of films was analyzed with x-
ray diffractometer (EXPERT-PRO) by using Cu-Kα lines (λ=
1.542Å). The average grain size in the fabricated films was
obtained from a Debye-Scherrer’s formula. Surface
morphology was examined by JEOL model JSM-6400
scanning electron microscope (SEM). The optical
transmission spectra for a rangeofsampleswereobtainedin
UV-VIS-NIR region using Perklin-Elmer UV-VIS lambda-35
spectrometer.[8-9].
RESULTS AND DISCUSSION:
Structural properties:
Figure1. shows the X-ray diffraction patternofZnSthinfilms
and ZnO thin film obtained from post annealing treatment
over ZnS films at various temperatures. The XRD pattern
confirms that the ZnS films get oxidized in the oven to form
ZnO thin films. It was found that cubic structured ZnS is
completely oxidizedathigherannealingtemperaturetoform
a hexagonal ZnO. The film shows reflections from (100),
(002) and (101) planes at 600°C, indicating the formation of
ZnO nano particles having pure hexagonal structure
(matches with JCPDF data) [9].
Meas. data:ZnS Sample1
Intensity(cps)
0
100
200
300
400
500
600
2-theta (deg)
Intensity(cps)
20 40 60 80
-100
-50
0
50
100
Meas. data:S1
Intensity(cps)
0
200
400
600
800
2-theta (deg)
Intensity(cps)
20 40 60 80
-100
0
100
Figure1. XRD patterns of ZnS and ZnO thin film fabricated at 600ºC
The average size of grain (g) have been obtained from the XRD patterns using Debye-Scherrer’s formula, [9]
g = Kλ / β cosθ ------------- (1)
Where,
K = constant taken to be 0.94, λ = wavelength of X-ray used (1.542Å), β = FWHM of the peak and θ = Bragg’s angle. The grain
sizes were found to be within the range from 08 to 43nm. This confirms the good crystallinity ofthesamples.Determinationof
Grain size and lattice strain of ZnS thin films are shown in Table1.
S. No. Sample 2 Theta (Degree) FWHM Value (Degree) Grain size (nm) Lattice strain
1 ZnS 1 59.89 1.17 8.19 0.0089
2 ZnS 2
32.62
32.295
37.077
48.263
57.31
63.55
68.56
0.22
0.199
0.262
0.27
0.37
0.30
0.47
39.31
43.43
32.97
33.69
25.56
37.089
27.36
0.0033
0.0030
0.0040
0.0026
0.0030
0.0015
0.0030
Table1: Determination of grain size & lattice strain of thin film sample
Surface Properties:
The surface morphology of deposited ZnO thin films were investigated by SEM at
different magnifications as shown in Figure 2.
Figure 2 Scanning Electron Micrograph of as deposited ZnO thin film at different magnification.
The deposits are compact, pinhole free with spherical grains from few nanometers up to clusters of 157 nm and the films are
well covered on the substrate. From the figure, it is observed that the small nanosized grains engaged in a fibrous- like
structure and nanoribbons which clearly indicates the nanocrystalline nature along with some amorphous phase of ZnO thin
films. The average grain size of the nanoparticles is about 130 nm. [10-11].
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1532
Optical Properties:
The optical energy band gap (Eg) was determined by plotting (αhν)2 versus hν and then extrapolating the straightlineportion
to the energy axis at α =0 (Figure 3). It was observed that the band gap of the film obtained at higher annealing temperature is
2.31eV [12-14].
Figure3. Plot of (αhν)2 vs hν for ZnO thin films fabricated at 600ºC
Effect of Deposition Temperature on Film Thickness:
Figure 4 shows the variation of film thickness as a function of deposition time at differenttemperatures.Varioustemperatures
from 3130K to 3450K in steps of 100K were used in the depositing ZnS & ZnO toobtaintheoptimal temperature.Figure4shows
an increase in film thickness as the temperature increases from 3130K to3450K.The riseinthefilmthicknessmaybe duetothe
dissociation of the Zinc-complexes (with ammonia and with thiourea) and increase in the hydrolysis of SC(NH2)2 as the
temperature increases. At higher temperatures, the decomposition of thiourea will be faster setting more S2- ions free.
Additionally, the Zinc-complex dissociation is greater and gives higher concentrations offreeZn2+ inthesolution,whichinturn
results in higher deposition rates or in other words for a constant buffer layer thickness, in shorter deposition times. Also the
kinetic energy of the ions in solution is higher at higher temperature, which brings about increased interaction between them
and subsequent deposition at volume nucleation centers of the substrate. It can be seen from figure,theaveragegrowthrateis
high at 345ºK (9.478nm/min) and it is slow at 313ºK (7.622nm/min). The prepared ZnS films werekeptintheoven atvarious
temperatures between 400ºC and 750ºC for 10 hours. The ZnS films get oxidized in the oven to form thin films of ZnO [15].
10 20 30 40 50 60 70 80 90 100
60
80
100
120
140
160
180
200
220
240
260
280
thickness(nm)
time(min)
40C
60C
70C
90C
30 40 50 60 70 80 90
50
100
150
200
250
300
thickness(nm)
deposition tem perature C
x=0.15 PH=10 R.P.M.=60/MIN R.T.=35C
FIGURE 4: Variation of film thickness as a function of deposition time at different temperatures.
CONCLUSION:
In present work we deposited ZnS andZnOmetal oxidesthin
films on different substrates by Chemical Bath Deposition
Technique. Structural, Surface Morphology and Optical
properties of as deposited films were investigated by XRD,
SEM, and UV-VIS Spectrophotometer. The X-ray diffraction
analysis showed that film is polycrystalline with pure
hexagonal structure. The grain size estimated is in the range
of 08 to 43nm. The band gap is also calculated from the
equation relating absorption co-efficient to wavelength.The
band gap indicates the film is transmitting within the visible
range and the band gaps changes because of the grain sizeof
the films. The film has a direct band gap withanoptical value
of 2.31eV which is in good agreement with the standard
value.
We also observed that, thechangein preparativeparameters
affects the deposition rate of thin films. From the
observation, it is clear that the growth rate increases as the
deposition temperature increases. This makes the films
suitable for various optoelectronic and sensor applications.
References:
[1] J. Y. Lao, J. Y. Huang, D. Z. Wang, Z. F. Ren, D. Steeves, B.
Kimball, and W. Poter, Appl. Phys.AMaterialsScience&
Processing, 78, 539, 2004;
[2] O. K. Varghese and C. A. Grimes, Journal of Nanoscience
and Nanotechnology, 3, 277, 2003.
[3] H. J. Fan, W. Lee, R. Scholz, A. Dadgar, A. Krost,
K.Nielsch,and M. Zacharias, Nanotechnology, 16,913,
2005.
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1533
[4] Y. Xia, P. Yang, Y. Sun, Y. Wu, B. Mayers, B. Gates, Y. Yin,
F. Kim, and H. Yan, Adv. Mater. 15, 353, 2003.
[5] P. A. Radi, A. G. Brito, J. M. Madurro, and N. O. Dantas
Brazilian J. of Physics, Vol.36, PP.412-414, 2006.
[6] J. P. Borah and K. C. Sarma, Acta Physica Polonica AVol.
114, No.4, 2008.
[7] M. Y. Nadeem, Waqas Ahme, Turk J Phy Vol. 24, PP.
651,2000.
[8] Jie Cheng, DongBo Fan, et al, Semicond. Sci. Technol.
Vol.18, PP. 676, 2003.
[9] S. S. Kawar, B. H. Pawar, Chalcogenide Letters, Vol. 6,
No. 5, p. 219 – 225, 2009
[10] B. S. Remadevi, R. Raveendran, A. V. Vaidyan,
Prammana J. Phy., Vol. 68, PP. 679,2007.
[11] G. K. Williamson, W. H. Hall, Acta Metall. Vol. 1, PP. 22–
31, 1953.
[12] J. J. Kelly, D. Vanmaekelbergh, in: G. Hodes (Ed.),
Electrochemistry of Nanomaterials, Wiley- VCH,
Weinheim, pp. 103–136, 2001.
[13] G. Cao, Nanostructure and Nanomaterials, first ed.,
Imperial College Press, London, 2004.
[14] P. X. Gao and Z. L. Wang, Journal of Applied Physics,
97,044304, 2005.
[15] K. K. Hurde, A. B. Lad, S. S. Kawar, B. H. Pawar,
International Journal of Materials Science, Volume 12,
Number 1, pp. 9-16 , 2017.

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Preparation and Properties of Nanocrystalline Zinc Oxide Thin Films

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume 4 Issue 4, June 2020 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470 @ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1530 Preparation and Properties of Nanocrystalline Zinc Oxide Thin Films S. S. Kawar Department of Physics, Shree Dr R G Rathod Arts and Science College, Murtajapur, Maharashtra, India ABSTRACT Metal oxide is highly important material whichpossesses manyuniqueoptical and electrical properties for applications in manyareassuchasSolarcells,Gas sensors and so on. With the developmentof researchand applicationsofMetal oxide thin films, research results are verified that the morphology of Metal oxide thin films are plays an important role in applications of these films. Variety of morphologies, complex structurehasbeendevelopedbyphysical or chemical methods. However the work on controlled growth of these films is still in developing state. Therefore in present work we deposited ZnSandZnO metal oxides thin films on different substrates by Chemical Bath Deposition Technique. Structural, Surface Morphology and Optical properties of as deposited films were investigated by XRD, SEM, and UV-VIS Spectrophotometer. The band gap isalsocalculatedfromtheequation relating absorption co-efficient to wavelength. The band gap indicates the film is transmitting within the visible range and the band gaps changes because of the grain size of the films. We also observed that, the change in preparative parameters affects the deposition rate of thin films. From the observation,itis clear that the growth rate increases as the deposition temperature, increases. KEYWORDS: Metal Oxide Thin films, Nanostructure, Chemical bath Deposition How to cite this paper: S. S. Kawar "Preparation and Properties of Nanocrystalline Zinc Oxide Thin Films" Published in International Journal of Trend in Scientific Research and Development(ijtsrd), ISSN: 2456-6470, Volume-4 | Issue-4, June 2020, pp.1530- 1533, URL: www.ijtsrd.com/papers/ijtsrd31623.pdf Copyright © 2020 by author(s) and International Journal ofTrendinScientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative CommonsAttribution License (CC BY 4.0) (http://creativecommons.org/licenses/by /4.0) INTRODUCTION: Electronic semiconductor devices and Photovoltaic devices are the main applications resultedinattremendous increase of innovative thin film processing technology. For the improvement of the technology, the materials of different properties and qualities are needed. The synthesis and characterization of various wide band gap metal oxide nanostructures such as nanowires, nanorods, nanobelts, nanobridges and nanowalls has attracted great interest due to their size, morphology related properties, and their emerging applications in novel functional nanodevices[1,2]. Recently, research and development of alternative energy technologies, such as low cost flatpanel solar cells thin film devices, and many otherinnovativeconceptshaveincreased. Metal Oxides such as ZnO, TiO2 is an important multifunctional material which has received great attention during the last few years due to their unique applications in microelectronic and optoelectronic devices, and for self- assembled growth of three dimensional nano scale systems [3, 4]. Metal oxide nano structures have the potential to significantly improve the performance and durability of certain devices used in areas of importance: energy production and homeland security. A key challenge in this research is to deposit nano structured metal oxide thinfilms with consistent morphology and reproducible properties with a long term stability. Therefore in present work we deposited ZnO metal oxide thin films on different substrates by Chemical Bath Deposition Technique. A nanostructured thin film of Zinc oxide (ZnO) have been obtained from Zinc sulphide (ZnS) films by annealing process in air at temperatures between 400ºC and 750ºC. The ZnS films have been fabricated onto glass substrates using simple & inexpensive chemical bath deposition technique (CBDT). The optical & structural characterization of obtained materials was performed. The x-ray diffraction (XRD) study has confirmedtheformation of ZnO with nano-size scale whereas the scanning electron microscopy (SEM) studies showed that all the films were polycrystalline in nature. Theoptical energybandgapsof the films were evaluated. The nano-crystalline materials exhibiting small particle size & large surface area may be applied for various gas sensors as well as in large area Optoelectronic devices. MATERIAL AND METHODS: To prepare ZnO films, aqueous solutions of zinc sources and thiourea with calculated proportion was added in 130 ml of de-ionized water. Complexing agent ammonia was added slowly to adjust the pH of the solution. The solution was stirred and transferred to another container containing substrate. The resulting solution was kept at 70±2ºC for 1 hour. The substrate used is commercial glass slide. Cleaning of substrate is important in fabrication of thinfilms,cleaning steps and growth procedure is reported elsewhere [5-7]. After 20-30 minutes the bath solution in beaker turned whitish, thus indicating the onsetZnSdepositionontheglass slide. After a reaction time of 1 hour the glass slides were taken out and dried in air for 15 minutes. Then for the post annealing treatment in air, the prepared ZnSfilms werekept IJTSRD31623
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1531 in the oven at various temperatures between 400ºC and 750ºC for 10 hours. The ZnS films get oxidized in the oven to form thin films of ZnO. The crystallographic structure of films was analyzed with x- ray diffractometer (EXPERT-PRO) by using Cu-Kα lines (λ= 1.542Å). The average grain size in the fabricated films was obtained from a Debye-Scherrer’s formula. Surface morphology was examined by JEOL model JSM-6400 scanning electron microscope (SEM). The optical transmission spectra for a rangeofsampleswereobtainedin UV-VIS-NIR region using Perklin-Elmer UV-VIS lambda-35 spectrometer.[8-9]. RESULTS AND DISCUSSION: Structural properties: Figure1. shows the X-ray diffraction patternofZnSthinfilms and ZnO thin film obtained from post annealing treatment over ZnS films at various temperatures. The XRD pattern confirms that the ZnS films get oxidized in the oven to form ZnO thin films. It was found that cubic structured ZnS is completely oxidizedathigherannealingtemperaturetoform a hexagonal ZnO. The film shows reflections from (100), (002) and (101) planes at 600°C, indicating the formation of ZnO nano particles having pure hexagonal structure (matches with JCPDF data) [9]. Meas. data:ZnS Sample1 Intensity(cps) 0 100 200 300 400 500 600 2-theta (deg) Intensity(cps) 20 40 60 80 -100 -50 0 50 100 Meas. data:S1 Intensity(cps) 0 200 400 600 800 2-theta (deg) Intensity(cps) 20 40 60 80 -100 0 100 Figure1. XRD patterns of ZnS and ZnO thin film fabricated at 600ºC The average size of grain (g) have been obtained from the XRD patterns using Debye-Scherrer’s formula, [9] g = Kλ / β cosθ ------------- (1) Where, K = constant taken to be 0.94, λ = wavelength of X-ray used (1.542Å), β = FWHM of the peak and θ = Bragg’s angle. The grain sizes were found to be within the range from 08 to 43nm. This confirms the good crystallinity ofthesamples.Determinationof Grain size and lattice strain of ZnS thin films are shown in Table1. S. No. Sample 2 Theta (Degree) FWHM Value (Degree) Grain size (nm) Lattice strain 1 ZnS 1 59.89 1.17 8.19 0.0089 2 ZnS 2 32.62 32.295 37.077 48.263 57.31 63.55 68.56 0.22 0.199 0.262 0.27 0.37 0.30 0.47 39.31 43.43 32.97 33.69 25.56 37.089 27.36 0.0033 0.0030 0.0040 0.0026 0.0030 0.0015 0.0030 Table1: Determination of grain size & lattice strain of thin film sample Surface Properties: The surface morphology of deposited ZnO thin films were investigated by SEM at different magnifications as shown in Figure 2. Figure 2 Scanning Electron Micrograph of as deposited ZnO thin film at different magnification. The deposits are compact, pinhole free with spherical grains from few nanometers up to clusters of 157 nm and the films are well covered on the substrate. From the figure, it is observed that the small nanosized grains engaged in a fibrous- like structure and nanoribbons which clearly indicates the nanocrystalline nature along with some amorphous phase of ZnO thin films. The average grain size of the nanoparticles is about 130 nm. [10-11].
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1532 Optical Properties: The optical energy band gap (Eg) was determined by plotting (αhν)2 versus hν and then extrapolating the straightlineportion to the energy axis at α =0 (Figure 3). It was observed that the band gap of the film obtained at higher annealing temperature is 2.31eV [12-14]. Figure3. Plot of (αhν)2 vs hν for ZnO thin films fabricated at 600ºC Effect of Deposition Temperature on Film Thickness: Figure 4 shows the variation of film thickness as a function of deposition time at differenttemperatures.Varioustemperatures from 3130K to 3450K in steps of 100K were used in the depositing ZnS & ZnO toobtaintheoptimal temperature.Figure4shows an increase in film thickness as the temperature increases from 3130K to3450K.The riseinthefilmthicknessmaybe duetothe dissociation of the Zinc-complexes (with ammonia and with thiourea) and increase in the hydrolysis of SC(NH2)2 as the temperature increases. At higher temperatures, the decomposition of thiourea will be faster setting more S2- ions free. Additionally, the Zinc-complex dissociation is greater and gives higher concentrations offreeZn2+ inthesolution,whichinturn results in higher deposition rates or in other words for a constant buffer layer thickness, in shorter deposition times. Also the kinetic energy of the ions in solution is higher at higher temperature, which brings about increased interaction between them and subsequent deposition at volume nucleation centers of the substrate. It can be seen from figure,theaveragegrowthrateis high at 345ºK (9.478nm/min) and it is slow at 313ºK (7.622nm/min). The prepared ZnS films werekeptintheoven atvarious temperatures between 400ºC and 750ºC for 10 hours. The ZnS films get oxidized in the oven to form thin films of ZnO [15]. 10 20 30 40 50 60 70 80 90 100 60 80 100 120 140 160 180 200 220 240 260 280 thickness(nm) time(min) 40C 60C 70C 90C 30 40 50 60 70 80 90 50 100 150 200 250 300 thickness(nm) deposition tem perature C x=0.15 PH=10 R.P.M.=60/MIN R.T.=35C FIGURE 4: Variation of film thickness as a function of deposition time at different temperatures. CONCLUSION: In present work we deposited ZnS andZnOmetal oxidesthin films on different substrates by Chemical Bath Deposition Technique. Structural, Surface Morphology and Optical properties of as deposited films were investigated by XRD, SEM, and UV-VIS Spectrophotometer. The X-ray diffraction analysis showed that film is polycrystalline with pure hexagonal structure. The grain size estimated is in the range of 08 to 43nm. The band gap is also calculated from the equation relating absorption co-efficient to wavelength.The band gap indicates the film is transmitting within the visible range and the band gaps changes because of the grain sizeof the films. The film has a direct band gap withanoptical value of 2.31eV which is in good agreement with the standard value. We also observed that, thechangein preparativeparameters affects the deposition rate of thin films. From the observation, it is clear that the growth rate increases as the deposition temperature increases. This makes the films suitable for various optoelectronic and sensor applications. References: [1] J. Y. Lao, J. Y. Huang, D. Z. Wang, Z. F. Ren, D. Steeves, B. Kimball, and W. Poter, Appl. Phys.AMaterialsScience& Processing, 78, 539, 2004; [2] O. K. Varghese and C. A. Grimes, Journal of Nanoscience and Nanotechnology, 3, 277, 2003. [3] H. J. Fan, W. Lee, R. Scholz, A. Dadgar, A. Krost, K.Nielsch,and M. Zacharias, Nanotechnology, 16,913, 2005.
  • 4. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD31623 | Volume – 4 | Issue – 4 | May-June 2020 Page 1533 [4] Y. Xia, P. Yang, Y. Sun, Y. Wu, B. Mayers, B. Gates, Y. Yin, F. Kim, and H. Yan, Adv. Mater. 15, 353, 2003. [5] P. A. Radi, A. G. Brito, J. M. Madurro, and N. O. Dantas Brazilian J. of Physics, Vol.36, PP.412-414, 2006. [6] J. P. Borah and K. C. Sarma, Acta Physica Polonica AVol. 114, No.4, 2008. [7] M. Y. Nadeem, Waqas Ahme, Turk J Phy Vol. 24, PP. 651,2000. [8] Jie Cheng, DongBo Fan, et al, Semicond. Sci. Technol. Vol.18, PP. 676, 2003. [9] S. S. Kawar, B. H. Pawar, Chalcogenide Letters, Vol. 6, No. 5, p. 219 – 225, 2009 [10] B. S. Remadevi, R. Raveendran, A. V. Vaidyan, Prammana J. Phy., Vol. 68, PP. 679,2007. [11] G. K. Williamson, W. H. Hall, Acta Metall. Vol. 1, PP. 22– 31, 1953. [12] J. J. Kelly, D. Vanmaekelbergh, in: G. Hodes (Ed.), Electrochemistry of Nanomaterials, Wiley- VCH, Weinheim, pp. 103–136, 2001. [13] G. Cao, Nanostructure and Nanomaterials, first ed., Imperial College Press, London, 2004. [14] P. X. Gao and Z. L. Wang, Journal of Applied Physics, 97,044304, 2005. [15] K. K. Hurde, A. B. Lad, S. S. Kawar, B. H. Pawar, International Journal of Materials Science, Volume 12, Number 1, pp. 9-16 , 2017.