A Statistical Approach to Optimize Parameters for Electrodeposition of Indium (III) Sulfide Films, Potential Low-Hazard Buffer Layers for Photovoltaic Applications
A Statistical Approach to Optimize Parameters for Electrodeposition of Indium (III) Sulfide Films, Potential Low-Hazard Buffer Layers for Photovoltaic Applications
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A Statistical Approach to Optimize Parameters for Electrodeposition of Indium (III) Sulfide Films, Potential Low-Hazard Buffer Layers for Photovoltaic Applications
1. Maqsood Ali Mughal
Environmental Sciences Proposal Defense
Room No. : 153
12:30 PM
Arkansas State
University
“A Statistical Approach to Optimize Parameters for
Electrodeposition of Indium (III) Sulfide Films,
Potential Low-Hazard Buffer Layers for Photovoltaic
Applications”
November 14, 2014
2. Why Solar Cells??
Rapidly falling
prices and gains
in efficiencies
Federal/state tax
incentives, and
rebates
World carbon
emissions rate is
projected to
increase to 11.0
GtC/yr by 2050 [3]
Fossil fuels are
not renewable
energy
Social
responsibility
Economic goals Sustainability
Source: beyond1energy, LLC
Source: beyond1energy, LLC
Energy reserves on
earth equals energy
from just 20 days of
sunshine [2]
Increased energy
demand, 18 TW by
2050 [1]
4. Role of Buffer Layer in Solar Cells
To form a junction with the absorber layer
while admitting a maximum amount of light
to the junction region and absorber layer.
To protect or passivate the junction material.
Provide layer of appropriate thickness and index of
refraction that will reduce the overall reflectance.
To absorb light energy from only the high-
energy end of the spectrum.
Must be thin enough and have a large enough
bandgap (2.3 eV or more) to let nearly all
available light through the interface
(junction) to the absorbing layer.
Photo taken by: John Hall
5. n-type
semiconductor
Large optical
bandgap of
(2.0-2.3) eV [4].
Stable, high absorption
coefficient, and
photoconductive [5][6].
Replacement for
hazardous CdS, as a
window layer in
solar cells [7].
Physical properties and structure of
In2S3 thin films
Structure Tetragonal
Color Yellow
Appearnce
Crystalline
solid
Melting Point 1050 oC
Density 4450 kg/m3
Lattice Parameters
a=b=7.619 Å
c=32.329 Å
Indium (III) Sulfide (In2S3)
6. Highest Efficiencies Achieved with In2S3-based Solar Cells Produced by
Various Deposition Methods
Buffer
Layer
Deposition
Method
Absorber
Layer
Efficiciency
[%]
Jsc
[mA/cm2
]
Voc
[mV]
FF
[%]
Area
(cm2
)
Reference Institution
In2S3
Sputtering CIGS 16.4 32.5 660 77.5 0.1 Naghavi N. et al. (2010) ZSW/HMI/WS
ALD CIGS 16.4 31.5 665 78 0.5
Naghavi N. et. al.
(2004)
ENSCP/ZSW
CBD CIGS 15.7 37.4 574 68.4 0.5 Allsop N.A. et al. (2005) IPE/ASC
PVD CIGS 15.4 33.7 628 72.7 0.528
Fraunhofe ISE
(2009)
Wurth Solar
ILGAR CIGS 14.7 37.4 574 68.4 0.5
Fischer C.-H. et al.
(2010)
HMI
ALE CIGS 13.5 30.6 604 73 N/A D. Lincot et al. (1995) LECA
USP CIGS 13.4 33.4 585 69 N/A Buecheler S. (2009) LTFP/SFLMTR
ED CIGS 9.5 29.3 535 61 N/A
Chassaing E. et al.
(2011)
IRDEP/IREM
CSP CuInS2 9.5* 48.2 588 33.5 N/A John T.T. (2005) CUSAT
Deposition
Method (Buffer
Layer)
Absorber
Layer
Buffer
Layer
Efficiency
[%]
Jsc
[mA/cm2]
Voc
[mV]
FF
[%]
Area
(cm2)
References
ALD
CIGS In2S3 16.4 31.5 665 78 0.5 A. Hultqvist, et al. 2007
CdTe CdS 16.7 32.8 671 75.8 0.5 Y. Yan, et al. 2012
CBD
CIGS In2S3 15.7 37.4 574 68.4 0.5
C. D. Lokhande, et al.
1998
CIGS CdS 20.8 39.6 581 60.3 0.5 P. Jackson, et al. 2014
PVD
CIGS In2S3 15.2 29.8 677 75.6 0.528 S. Gall, et al. 2007
CIGS CdS 14 31.4 613 73 0.5 U. P. Singh, et al. 2010
Sputtering
CuInS2 In2S3 12.2 31.5 665 78 0.1 N. Naghavi, et.al, 2003
CuInS2 CdS 9.4 20.3 671 68.9 0.5 A. Grimm, et al. 2008
USP
CIGS In2S3 11.9 30.2 543 73 0.3 N. Demirci, et al. 2012
CIGS CdS 12.5 30.3 576 73 0.3 Fella, et al. June 2010
Electrodeposition
CIGSe In2S3 10.4 29.3 535 61 0.5 N. Naghavi, et al. 2011
CdTe CdS 10.8 23.6 753 61 0.5 S. K. Das, et al. 1993
In2S3 vs. CdS
7. Electrodeposition 1) Straightforward scale-up to
larger areas.
2) Low cost, simple apparatuses
and reagents; no vacuum
required [8].
3) Relatively low hazard due to
non-gaseous nature.
4) Potential for stoichiometry
control through variation of
deposition voltage and current, and
in-situ monitoring of photocurrents.
5) Excellent material utilization
efficiency [9].
Three-electrode
Electrochemical Cell
Side View
Aerial View
Coated-glass
substrate
(cathode)Reference
electrode
Graphite
(anode)
Magnetic
stir bar
Teflon
cover
Temperature
probe
Glass Beaker
8. Experiment Details
Solvent: ethylene glycol, 150 ml
Solutes: 0.1 M NaCl, 0.1 M Na2S2O3. 5H2O, 0.05 M InCl3
(Sulfur concentration is 0.1 M and 0.15 M)
Anode (counter electrode): graphite, 1.25 inch by 1.25 inch.
Reference electrode: Ag/AgCl (filled with KCL & C2H6O2)
Cathode (working electrode): molybdenum-coated glass, ITO, FTO
Thickness: 0.12 inch
Material: SiO2: Mo
Target resistivity value of 2.5 – 30 ohms per square
Size: 1 inch by 1 inch
Wavenow digital potentiostat: Pine Research Instrumentation
Digital hotplate from Fisher Scientific (Isotemp 11-400-49SHP)
was used to heat and stir the solution.
Substrates ultrasonically (Cole Parmer 8890) cleaned with
acetone for 15 min
Distilled water used for rinsing the films
* Samples are stored in air-tight plastic boxes/bags to protect the films.
13. Why Taguchi Experimental Design?
Taguchi Methods are statistical methods developed
by Genichi Taguchi to improve the quality of manufactured
goods, and more recently have also been applied to
engineering, biotechnology, etc [10].
Two basic goals of Taguchi Methods:
Quality Control
Design of Experiments (DOE)
To determine the “best” combination of factors and levels to produce
a high quality product.
To measure the impact/sensitivity of factors and parameter levels on
the characterized performance of a product using statistical analysis
tools (Orthogonal Regression, ANOVA, etc.).
14. Analyzing
Experimental Data
Once the design of experiments (DOE) has
been determined and the trials have been
conducted, the measured performance
characteristic from each trial can be used to
analyze the relative effect of the different
parameters.
To demonstrate the data analysis procedure,
the following orthogonal design arrays (L18,
L27, etc.) will be used, but the principles can be
transferred to any type of array.
The Taguchi Method allows for the use of a
noise matrix including external factors
affecting the process outcome rather than
repeated trials [11].
Software:
Minitab, Matlab, MS Excel
і = experiment number
u = trial number
Ni = number of trials for experiment i
S/N
15. Collected : 14-Sep-2011 06:15 PM
Livetime (s) : 37.16
Real time (s) : 38.30
Detector : Silicon
Window : SATW
Tilt (deg) : 0.0
Elevation (deg) : 45.0
Azimuth (deg) : 0.0
Magnification : 552 X
Accelerating voltage ( kV ) : 19.48
Process time : 4
EDS Elemental Peaks for In2S3
16. SEM/EDS Analysis
Spectrum 1
Spectrum 2
Spectrum 3
(a) (b)
Experiment No. 5 and Trial No. 2) (a) SEM image of In2S3 film at 1.21 kX (b) SEM image of
scratched-off film on an aluminum stub at 99 X with selected surface area (squares) for EDS
analysis
20. Orthogonal Regression Analysis
(S/In vs. Deposition Voltage)
Plot of S/In Ratio vs. Deposition Voltage with Fitted Line
S/InRatio
Deposition Voltage (V)
21. Spectrum In stats. O Si S Mo In Total S/In
Spectrum 1 Yes 6.54 0.00 54.1 3.12 36.24 100.00 1.493
Spectrum 2 Yes 0.00 0.00 56.65 8.36 37.51 100.00 1.51
Spectrum 3 Yes 0.00 0.00 55.18 7.27 37.54 100.00 1.471
Spectrum 4 Yes 14.48 0.00 50.65 2.82 33.75 100.00 1.5
Spectrum 5 Yes 0.00 0.00 58.32 0.00 40.5 100.00 1.443
Spectrum 6 Yes 0.00 0.00 59.8 0.00 39.91 100.00 1.498
Spectrum 7 Yes 4.21 0.00 57.49 0.00 38.30 100.00 1.501
Spectrum 8 Yes 0.00 0.00 60.28 0.1 39.71 100.00 1.53
Mean 1.493
Max. 14.48 0.00 60.28 8.36 40.5
Min. 0.00 0.00 50.65 0.00 33.75
MM-In2S3-09/01/11-6
EDS Data for In2S3 Films Grown at Optimal Values Obtained
from Taguchi Analysis
22. Morphology- Scanning Electron Microscopy
(SEM)
Electrodeposited at -
0.685 V for 6 min. and at
-0.7 V for 40 min.
(repeated trials)
Pulse-plating (-0.8 V
with 10 sec. delay) at120
oC for 50 min. Mo
Pulse-plating (-0.685 V
with 10 sec. delay) at 70
o
C for 95 min. FTO
Pulse-plating (-0.7 V
with 15 sec. delay) at 150
oC for 48 min. FTO
Pulse-plating (-0.7 V
with 10 sec. delay) at 80
oC for 75 min. ITO
Indium sulfide ring
formation from sodium
thiosulfate as sulfur
source-ITO
Electrodeposited at -
0.685 V for 4 min with
ethylene glycol solvent
Current density:
0.75 mA/cm2
Electrodeposited at -0.7
V for 15 min. (sodium
thiosulfate as sulfur
source)
Electrodeposited at -0.7
V for 50 min. at 160 o
C
JH: Electrodeposited at -
0.8 V for 30 min in
formamide solvent
Current density:
1.25 mA/cm2
Current density:
1.5 mA/cm2
Current density:
1 mA/cm2
Low resistance substrate-
ITO at150 o
C
Electrodeposited at -0.7 V for
50 min. at 160
o
C
Indium sulfide ring formation
from sodium thiosulfate as
sulfur source-ITO
Electrodeposited at -0.7 V for
15 min. (sodium thiosulfate as
sulfur source)
Post-annealed
electrodeposition
Post-annealed
electrodeposition
(repeated trials)
Post-annealed electrodeposition Post-annealed electrodeposition
(repeated trials)
Horizontally positioned
substrate-Mo
Horizontally positioned substrate-
MoLow resistance substrate-ITO at150
o
C
Pulse-plating (-0.685 V with 10 sec.
delay) at 70
o
C for 95 min. FTO
Pulse-plating (-0.7 V with 15 sec.
delay) at 150 oC for 48 min. FTO
Pulse-plating (-0.7 V with 10 sec.
delay) at 80 oC for 75 min. ITO
Electrodeposited at -0.685 V for 6
min. and at -0.7 V for 40 min.
(repeated trials)
Electrodeposited at -
0.685 V for 4 min using
ethylene glycol solvent
JH: Electrodeposited at -0.8 V for 30 min
in formamide solvent
Current density:
0.75 mA/cm2
Current density: 1.25 mA/cm2Current density: 1.5 mA/cm2
Pulse-plating (-0.8 V with 10 sec. delay)
at120 oC for 50 min. Mo
Current density:
1mA/cm2
23. Reported Papers on Electrodeposition of Semiconductor
Thin Films with Crack Morphology
Semiconductor
Material
Electrolyte Potential Cause for Cracks Reference
CdS Organic Thickness and current density Fulp & Taylor, 1985
CdS DEG-water mixtures
Incorporation of solutes with solvent/addition
agent
Fulp & Taylor, 1985
Si Ionic Liquid Thickness, substrates, deposition voltage Oskam et. al., 2001
Bi2S3 Aqueous Solvents A. Begum, et al. 2011
CIGS Aqueous % composition of precursor chemicals V. S. Saji, et al. 2011
CdS Organic Solvent and piezoelectric effect
M. N. Mammadov, et al.
2012
Cu-Ga-Se Aqueous
Incorporation of solutes with solvent/addition
agent and % composition of precursor
solutions
Y. Oda, et al. 2008
Cu Aqueous Surface contamination
H. Lou & Y. Huang,
2006
CdSe Aqueous Substrates
R. I Chowdhury, et al.
2011
24. Crack Morphologies from Solution-Based Deposition
Techniques
Cu-Ga-S (Y. Oda, et al.
2008)
CZTS(M. Jiang and X. Yan
2008)
TiO2 (A. R. Santos, et al.
2013)
ZnO (C. Liehiran, et al.
2007)
Ƴ-Fe2O3 (AT. Ngo, et al. 2013)
ZnO:Cl on CIGS/In2S3 (J.
Rousset, et al. 2011)
TiO2 (G. Xue, et al. 2012)
In2S3 (K. Otto, et al. 2011)In2S3 (E. Aydin, et al.
2012)
25. Control Deposition Parameters and Levels
Levels “A”
Bath Composition
“B”
Current
Density
(mA/cm2)
“C”
Substrate
“D”
Deposition
Time
(min)
“E”
Deposition
Temperature
(oC)
1 0.1M S + 0.05M InCl3 +
0.1M NaCl
0.75 Mo 5 140
2
0.1M S + 0.1M
Na2S2O3.5H2O +0.05 M
InCl3 + 0.1M NaCl
1.25 ITO 10 150
3 ----- 1.75 FTO 15 160
26. Digital Imaging Analysis: Fracture and Buckling
Analysis Software for Crack Density Calculation
(Area of interest = 2100.69 µm2)
32. Future Work
i. Study and improve the crystalline structure of In2S3 films as a function of heat treatment
and then compare the results from conventional oven-based heating versus laser
annealing, and intense pulse light annealing.
ii. Use the X-ray mapping feature on the EDS to study elemental distributions over the
surface area of the electrodeposited In2S3 films.
iii. Study the effect of performance parameters as a function of thickness of In2S3 films.
iv. Prepare/complete three potential papers for publication:
- Effect of different heat treatments on the crystalline structure of electrodeposited In2S3
films.
- Indium Sulfide: A Review
(The paper will feature all of the In2S3-based solar cells with record efficiencies produced
with various deposition techniques).
- Life Cycle Assessment (LCA) of In2S3-based solar cells.
33. 1) M. A. Mughal, M. J. Newell, R. Engelken, B. Ross Carroll, J. Bruce Johnson, et al.,
"Statistical analysis of electroplated indium (III) sulfide (In2S3) films, a potential
buffer material for PV (heterojunction solar cell) systems, using organic
electrolytes," Nanotechnology 2013: Bio Sensors, Instruments, Medical,
Environment, and Energy,3. Technical Proceedings of the 2013 NSTI
Nanotechnology Conference, Washington, DC, pp. 523-527, May 12-16, 2013.
2) M. A. Mughal, M. J. Newell, R. Engelken, B. Ross Carroll, J. Bruce Johnson, et al.,
“Morphological and compositional analysis of electrodeposited In2S3 Films”
Proceedings of the 40th IEEE Photovoltaic Specialists Conference (PVSC),
Denver, CO, pp. 1322-1326, June 07-14, 2014.
3) M. A. Mughal, M. J. Newell, R. Engelken, B. Ross Carroll, J. Bruce Johnson, et al.,
“Optimization of the electrodeposition parameters to improve the stoichiometry
of In2S3 films for solar applications using the Taguchi Method, Journal of
Nanomaterials, vol. 2014, pp. 1-10, 2014.
4) Paper submitted (October, 2014) to IEEE Journal of Photovoltaics (under review)
on “Morphological and compositional analysis of electrodeposited In2S3 films”.
Scholarly Publications
35. 1) Poster presentation at Fourth Annual Renewable Energy Conference (Sep., 2014) on “Update on Semiconductor Film
Electrodeposition Research at Arkansas State University”, Arkansas State University-Jonesboro, AR.
2) Posterl presentation at ASSET Initiative Annual Meeting (Sep., 2014) on “Update on Semiconductor Film
Electrodeposition Research at Arkansas State University ”, Little Rock, AR .
3) Poster presentation at 40th IEEE PVSC Conference (June, 2014) on “Morphological and Compoitional Analysis of
Electrodeposited In2S3 Films”, Denver, CO.
4) Poster presentation at TechConnect Conference (May, 2013) on “Statistical Analysis of Electroplated Indium (III) Sulfide
(In2S3) Films, a Potential Buffer Material for PV (Heterojucntion Solar Cells) Systems, using Organic Electrolytes”,
Washington, DC.
5) Poster presentation at Create@State (Apr., 2013) on “Innovations in Semiconductor Electrodeposition”, Arkansas State
University, Jonesboro, AR.
6) Poster presentation at Arkansas State Capitol (Feb., 2013) on “CdTe/In2S3 Solar Cells by Electrodepostion and
Evaporation”, Little Rock, AR.
7) Oral presentation at ASSET Initiative Annual Meeting (Aug., 2012) on “Progress and Challenges in Electrodeposition of
Indium (III) Sulfide (In2S3) Films from Organic Electrolytes for Potential Solar Cell Use”, Springdale, AR.
8) Oral presentation at Arkansas Academy of Science ( Apr., 2012) on “Taguchi Analysis and Characterization of
Electrodeposited Indium Sulfide Films for Use as Potential Buffer Layers in Solar Cells”, Magnolia, AR (Third prize in the
graduate physics category).
9) Oral presentation at Create@State (Apr., 2012) on “Rest Potential-Based Electrodeposition of Metal Sulfide Films”,
Arkansas State University, Jonesboro, AR.
10) Poster presentation at Arkansas State Capitol (Feb., 2012) on “Progress in Electrodeposition of Indium Sulfide and Copper
Indium Disulfide”, Little Rock, AR.
11) Poster presentation at ASSET Initiative Annual Meeting (July, 2011) on “Research at Arkansas State University
Optoelectronic Materials Research Laboratory”, Heber Springs, AR.
12) Oral presentation at Electronic Materials Conference EMC (June, 2011) on “Electrodeposition of Indium Sulfide Films
from Organic Electrolyte”, University of Santa Barbara, Santa Barbara, CA.
13) Oral presentation at Create@State (Apr., 2011) on “Electrodeposition of Indium Sulfide from Organic Electrolytes”,
Arkansas State University, Jonesboro, AR.
14) Oral presentation at Arkansas Academy of Science ( Apr., 2011) on “Elemental Sulfur-based Electrodeposition of Indium
Sulfide Films”, Monticello, AR (First Prize in graduate category).
Scholarly Activities
36. I acknowledge the gracious support provided by Arkansas State University,
National Science Foundation grant EPS-1003970 administered by the Arkansas
Science and Technology Authority, and NASA grant NNX09AW22A
administered by the Arkansas Space Grant Consortium. Dr. Alan Mantooth,
Kathy Kirk, Dr. Greg Salamo, Dr. Omar Manasreh, Dr. Alex Biris, Dr. Tansel
Karabacak, Dr. Hyewon Seo, and other collaborators at the University of
Arkansas (Fayetteville, Little Rock, and Pine Bluff campuses) are also thanked,
as are Dr. Keith Hudson and Laura Holland at ASGC, and Dr. Gail McClure, Cathy
Ma, and Marta Collier at ASTA. The authors are also grateful for the ongoing
support provided by Arkansas State University, particularly Dr. David Beasley,
Dr. Rick Clifft, Dr. Paul Mixon, Dr. William Burns, Dr. Tom Risch, Dr. Tanja McKay,
Dr. John Pratte, and Dr. Andrew Sustich.
Thanks also go to Dr. Richard Segall and Dr. Ilwoo Seok for an introduction to
the Taguchi Method, and Dr. Trauth for the use of the SEM/EDS unit.
Particular thanks go to my advisor, Dr. Robert Engelken, my student research
colleagues, and all of you, my Ph.D. committee members.
Thank You !
Acknowledgements
37. References
1) Roy L. Nersesian. 2007. Energy for the 21st Century: A Comprehensive Guide to Conventional and
Alternative Sources / Roy L. Nersesian. n.p.: Armonk, N.Y.: M.E. Sharpe.
2) George Greenstein. 2013. Understanding the Universe: An Inquiry Approach to Astronomy and the
Nature of Scientific Research. Cambridge University Press.
3) Dr. Pieter Tans, NOAA/ESRL (www.esrl.noaa.gov/gmd/ccgg/trends/), and Dr. Ralph Keeling, Scripps
Institution of Oceanography (scrippsco2.ucsd.edu/). Available at:
http://www.esrl.noaa.gov/gmd/ccgg/trends/
4) M. Lajnef and H. Ezzaaouia. 2009. “Structural and Optical Studies of Indium Sulfide Thin Films
Prepared by Sulfurization of Indium Thin Films.” The Open Applied Physics Journal, 2, pp. 23-26.
5) A. M. Abdel Haleem, M. Sugiyama, and M. Ichimura. 2012. “Sulphurization of the Electrochemically
Deposited Indium Sulphide Oxide Thin Film and its Photovoltaic Applications.” Materials Sciences and
Applications, vol. 3, no. 11, p. 802.
6) T. T. John, S. Bini, Y. Kashiwaba, T. Abe, Y. Yasuhiro, C. Kartha, and K. Vijaykumar. 2003.
“Characterization of Spray Pyrolysed Indium Sulfide Thin Films.” Semiconductor Science and
Technology, vol. 6, pp. 491-500.
7) Walther Schwarzacher. 2006. “Electrodeposition: A Technology for the Future.” The Electrochemical
Society Interface, pp. 32-33.
8) Milan Krenzelok, Petr Rychlovsky, Michael Volnya, and Jaroslav P. Matouse. 2003. "Evaluation of In-Situ
Electrodeposition Technique in Electrothermal Atomic Absorption Spectrometry." Analyst , 128.3, pp.
293-300.
9) I. N. Vuchkov and L. N. Boyadjieva. 2001. Quality Improvement with Design of Experiments: A
Response Surface Approach. Kluwer Academic Publishers. Dordrecht, 2001.
10) D. M. Steinberg and D. Burnsztyn. 1998. “Noise Factors, Dispersion Effects, and Robust Design.”
Statistica Sinica, vol. 8, pp. 67-85.
Editor's Notes
Thank you everyone for coming in today, especially my committee members, my advisor, Dr. Engelken, and Dr. McKay for taking time off their busy schedules. I am Maqsood Ali Mughal and Today I am defending my PhD. Proposal.. I also like to say thanks to my sponsors, NSF through victer and ASSET initiative, NASA epscor for first two years of my Ph.D, without them this research would not have been possible. So, lets start with the presentation, my research is on a semiconductor material called In2S3 which we believe has the potential to replace the hazardous CdS in solar cells and therefore, the title for the presentation is a A Statistical Approach to Optimize Parameters for Electrodeposition of Indium (III) Sulfide Films, Potential Low-Hazard Buffer Layers for Photovoltaic Applications”.
Why solar cells? Now there are many reasons that why we should switch to solar energy, I short listed top six important reasons that I thought explain very well that why we need to switch our gears. (1) Today, we are providing energy to roughly 7 billion people on earth, however, population is predicted to increases to 9.4 billion by 2050 and therefore we will require 18 TW of energy in future and this number triple by 2100. So we need more sources or energy. So if you look at this map, you will see three different size of square boxes, smallest one representing roughly a surface area of 200,000 sq km, the largest one around 500,000 sq km, and the medium sized one around 300,000 sq km. These 19 distributed areas on the map show roughly what would be a reasonable responsibility for various parts of the world to create energy from sunlight that will feed the whole planet.(2) Coal, oil, and natural gas supply 88% of world energy needs. The sun can provide us enough energy in one hour that can feed the whole planet. And the map you see is an evidence that there is clearly a lot of solar energy potential. There are plenty of orange and red zones (South America, Africa, Australia, North America, SUbcontinet) where solar radiation is more than 1600 kw/m2/yr. (3) Renewable energy technology (RET) has improved and is more affordable than it was 25 years ago. Not just solar but prices for wind and geothermal have also decreased. The wind energy is available for 5₵/ kilowatt-hour (kWh) which is an 800% decrease in cost from 2001 (Phillipe 2003). The solar energy cost has declined from $1.25/kWh in 1980 to 11₵/kwh in 2013. Similarly, efficiencies have improved and NREL just introduced a solar cell which is 20.8% efficient and Sharp came up with a multijunction solar cell with conversion efficiency of 44%. (4) For example in California, with 30% federal tax return and 20% state tax return or other initiavtes, your payback period could be as low as 6 years. (5) Solar cells can diminish the fossil fuel energy consumption and therefore reducing the dependency on foreign oil, but also the environmental pollution and, consequently, the climate change. (6) Once they are gone, they are gone.
Switching to solar panels will allow us to be socially responsible by using clean energy and not polluting our environment. Solar energy after installation is INFLATION FREE source of power, which means you are not dependent on fluctuating raw material cost for your generation of power...This adds to energy independence. In countries where power is not reliable, we can opt for green source of energy to replace diesel generators or battery backup. Which then help us achieve sustainability.
http://www.sandia.gov/~jytsao/Solar%20FAQs.pdf
http://solarword.blogspot.com/2012/10/the-reasons-why-should-we-switch-to.html
I like to give information on the solar structure. you have back contact (a transparent conducting oxide, such as tin oxide. These oxides are highly transparent and conduct electricity very well), p-type semiconductor on top of it, also known as absorber layer in which photons from sunlight are efficiently absorbed result in the creation of electron-hole pairs. N-type semiconductor also known as buffer layer or window layer, ideally you want this layer to transmit all the light to the p-type absorber for maximum absorption.
So when radiations from sunlight strikes the solar panel, absorption of those radiations raises an electron to a higher energy state, and secondly, the movement of this higher energy electron from the solar cell into an external circuit. The electron then dissipates its energy in the external circuit and returns to the solar cell. When electron moves to a higher energy state it leaves a hole and eventually after loosing its energy recombines with the hole. On the right is a solar structure for one of the most popular solar cell today.
When the light strikes the P-substrate, it excites an electron. This electron either is absorbed back into the P-substrate, or it can move into the N-substrate and gets absorbed there. Once the electron has moved into the N-substrate, due to the PN junction, the easier path to balance the charges is to push electrons through an external circuit. Passivation prevents surface recombination of minority carriers. Improves interface properties.
It is an indirect bandgap semiconductor material with a bandgap of 2.2 eV. It features good absorption, photconductivity with potential to replace hazardous cadmium sulfide. Cadmium is a sixth most toxic element on earth and is difficult to market since it is banned in EU countries and countries like China. The Beta phase indium sulfide has a tetragonal structure and appears to have yellowish orangish color with high melting point above 100 degree centigrade.
There have been various efficiencies reported for In2S3 based solar cells from various deposition methods with highest being 16.4% reported by ecole National lab in Paris. Films were deposited using atomic layer deposition technique. Also, down at the bottom of the table we have electrodeposited In2S3 that yeilded an efficiency of 9.5% reported by Institute of Research and Development on Photovoltaic Energy. So there is a room for improvement in the case of electrodeposition. This is a compariosn of recorded operational performance of In2S3 vs. CdS-based solar cells fabricated by different deposition techniques. The overall performances of the devices made from these buffer layers are very close, and the numbers further converge as there is more research focusing on In2S3.
This is a key component of my research, electrodeposition. Indium sulfide films are deposited by electrodeposition technique due to following reasons:
So If you look at the picture on bottom right, this is how the electrochemical cell looks from inside. Basically, you have two electrodes inside, a negative potential or voltage is applied across the electrodes which then creates an electric field in the solution that drives ions. There is a reduction reaction i.e. gain of electrons that takes place at the surface of the cathode and that leads to the deposition of the material. But, but believe me it is complex in a way that there are so many deposition parameters involved that you really need to optimize them.
Early on when I started working on this project. I was growing films at random electrodeposition parameters and I used to analyze the performance parameters based on those parameters. For example, this experiment was performed on 14th Feb, 2014, here is the composition and deposition parameters, and here is the bandgap, thicknesses, stoichiometries, for all these films. This allowed me design experiments with parameters and levels where there is a good chance to optomize them and improve the performance of the material.
Here are few pictures from some of preliminary experiments. ITO’s, FTO’s, Molybdenum and Titanium Foils, etc.
Just go through. I have used different solvents including Dimethyl sulfoxide, tetraethylene glycol, dimethyl formamide, triethylene glycol, and mixed solvents. I had most luck with ethylene glycol.
Just go through. Absorbance using which you can calculate optical bandgap. Stoichiometry, the composition of film in terms of sulfur and indium content. Crystallinity, morphology, and thickness of the In2S3 films.
Just to give a little background on Taguchi Method. It was developed by Genichi Taguchi who worked in Bell labs in 1950’s and proposed this statistical technique to improve the quality of a product. The primary goals of TM are quality control and design of experiment. So, the deal was using this I was able to find the optimal electrodeposition parameters.
Once you have completed all the experiments, it is time to analyze the data. For this you choose a performance parameter for example stoichiometry for which you analyze the relative effect of the different parameters. The Taguchi Method will allow the use of a noise matrix including external factors affecting the process outcome rather than repeated trials. So not just you save time but you save money on material. The formula to calculate signal to noise ratio for each performance parameter is right here, where y is the mean value of the performance value and s is the variance. Since we had more than one trial for each experiment I is the experiment number and u is the trial number and Ni is the number of trials for each experiment.
One issue that we have when obtaining sulfur and indium compositions in In2S3 films from EDS was the k-Alpha values (binding energy) for molybdenum and sulfur are so close to each other that molybdenum peak would coincide with sulfur peak.
So to eliminate that issues Dr. Engelken suggested me to scratch off films from molybdenum substrate and then do analysis. So, I scratched-off In2S3 films and collected it in a powder form on an aluminum stub. So here is you see a SEM image of a film and on the right you see a scratc film where this grey area is the aluminum stub, black is the adhesive on the stub, and white is the indium sulfide powder.
So, sulfur to indium ratios were obtained from energy dispersive x-ray sppectroscopy. The solid black squares represents the films which were uniform while rest of the films were non-uniform. For each experiment, I conducted three trials, therefore a total of 81 experiments were performed and films were then analyzed. Here are the S/In ratios for each trial and a mean.
So here is the output response table for signal-to-noise ratios. Like I said the output response for this study was stoichiometry of Indium sulfide films. The four deposition parameters and SN ratios calculated for them are listed here. The solid triangle here is called as delta which is the difference between highest SN ratio and lowest SN ratio for each parameter. And then you rank them in the increasing order. Deposition voltage being the highest significant factor and deposition temperature being the least significant factor to have an impact upon stoichiometry for films.
This graph basically tells the same thing but it also tells the optimum value for each deposition parameter and the combination of four are the optomized electrodeposition parameters that can produce a quality film with proper stoichiometry.
Orthogonal regression analysis helped improve mean characteristic performance value and drive it closer to the target value, thus improving the quality of the product. For example, S/In has ratio of 3 is to 2,i.e. 1.5 and this analysis predict that we can achieve that ratio if we grow our films at -0.685 V potential.
So I grew the films at -0.685 V. The film was analyzed using energy dispersive spectroscopy to find the stoichiometry of In2S3 films. To achieve accuracy and confirm the composition analysis was performed on 8 different areas over the sample. The proper stochiometry was achieved and the mean stoichiomettric ratio between sulfur and indium was 1.49 extremely close to the target value.
Morphology is an important characteristic of any thin film with high stability and performance for solar applications. Synthesizing thin films via solution deposition techniques like electrodeposition has the potential for crack formation, pinholes, or blisters resulting from larger deposition rate [21], mass transport [22], thickness [23], Therefore, surface morphologies of the In2S3 films were characterized by scanning electron microscopy. And that you will see here on this slide that the morphology is dependent upon several parameters: (1) For example, this film was grown on ITO glass with high deposition temperature and large deposition time at -0.7 V. The film appeared to be uniform but with cracks. (2) This film was grown using a manually controlled potentiostat and adding sodium thiosulfate later on in the solution to use as an additional sulfur source.(3) For this film the deposition time was only 15 minutes, so you are looking at a magnification scale of 10 kx. This is a sulfur particle on the film, it is hard to dissolve sulfur uniformly and therefore the stir rate and high temperatures are crucial to avoiding these sulfur particles on the film. It also happens when film is not properly rinsed with water. (4,5)The films were grown by repeated trials, the idea was to fill up those void gaps on the films by repetitive electrodeposition of In2S3 films. But the idea flopped as it grew a crack film over a crack film, the film would flake-off of the substrate. (6) In this case the substrate was horizontally placed at the bottom of the beaker using a platinum wire and the film was grown it. The result was a non-uniform In2S3 film that also exhibited cracks. Since, I couldnot stir my solution because susbtrate was lying on the bottom of the beaker and therefore you see sulfur particles on the film.(7) Low resistant substrates were used to see if films turn out smooth, uniform, and adherent, but result was disappointing. (8.9,10,11) In the typical electroplating process, direct current (DC) is supplied to the plating bath as straight DC current. In pulse plating, the DC power arrives in the bath in a series of short pulses. The idea behind pulse plating was to improve conductivity, distribution of the solutes, lower porosity increasing layer density, higher density, greater throwing power, and less metal usage. Different substrates were used and The films looked very nice, the appearance was pleasant to eye but not when looked at microscopic scale. Overall, with this technique films exhibited fewer cracks but there were cracks. One thing that is very interesting here and is also consistent throughout is that these sulfur particles likes to settle down and hide between these cracks. (12,13)Different solvents were used, different deposition times, and temperatures, substrate types were used but to no vain. (14)Few years ago before I started on this material John Hall use to work on it and I took one of his old sample and did SEM on it and I found similar crack formation. He was plating films at -0.8V and using formamldehide as a solvent. (15,16,17,18) It was until I found about current density that has a high potential to cause cracks in thin films, I started growing films at various current densities and I found that lower the current density lower is your crack density. Actually at -0.75 mA.cm2 I was able to grow a crack-free film.
SSo after achieving the proper stoichiometry, I wanted to improve the morphology of my samples. Like I just showed you all that the films have cracks, which form porous zones on the substrate [26] [29] and could possibly result in the loss of charge carriers and insufficient electrical transport within the PV cells. So I did a literature review and I found papers on electrodeposition of semiconductors thin films with crack morphology. And here are the potential causes for cracks reported that includes…read through …
Similarly, I found SEM images for thin films with crack morphology from solution-based deposition techniques that featured cracks similar to the ones on my films.
So, all this literature available helped to set up another project which would be to eliminate the cracks without compromising on key efficiency parameters of the films. So, for this project the control deposition parameters and levels were…read through..
The idea was to calculate the crack density of In2S3 films and use it as an output response for Taguchi Analysis and determine the optomized electrodeposition parameters in order to achieve crack-free films and with proper stocihiometry. We simulate our results using fracture and buckling analysis software, to calculate mean crack density and cumulative/mean distance between cracks of In2S3 films. This analytical program helps to determine crack density of thin films at the micro/nano-scale by digital analysis of SEM images in a reasonable amount of time with high accuracy. was written using MATLAB Version 7.1 (R14). It investigates and detects the dark features of the image (as seen in Fig. 3. In green) compared to the average intensity of the image in few minutes time. The crack density is determined by linear analysis. A line pattern (in blue) over the selected area of interest is superimposed onto the SEM image, where this line pattern is perpendicular to cracks. The intersections between the analysis lines and cracks are determined. Hence, the crack density is determined by dividing the number of intersections with the cumulative line length [20]. The red dotted box indicates the area of interest, which is approximately 2100.69 µm2 (54.62 µm x 38.46 µm). The red box displays the crack density and distance between cracks for a film.
This is the output response for means. Again delta here is the difference between the highest mean and the lowest mean. And you rank them in increasing order. Therefore, current density was the most significant factor in terms of eliminating cracks and that composition has the least significant impact upon the crack density of In2S3 films.
And This graph basically tells the same thing but it also tells the optimum value for each deposition parameter and the combination of five are the optomized electrodeposition parameters that can produce a quality film with no cracks. However, I had to decrease the deposition time to 5 minutes to grow thinner films. Films with thickness above 350 nm exhibited cracks.
I also calculated the S/In ratio for the optomized In2S3 films and they were thermally treated in a heating oven at three different temperatures. Since the films were slight sulfur rich, the idea was to evaporate excess sulfur by annealing the sample. At 300oC we obtained the proper stoichiometry. However, the films contained a higher percentage of oxygen due to oxygen substituting with sulfur to form In2S3-xOx during the process
The films have shown a bandgap of around 2.2 eV which is consistent with the literature.
The films have also shown beta-phase crystallinity. Unfortunately, due to unavailability of XRD, I have not been able to run my samples on X-ray diffraction. However, my future research greatly depends upon using XRD and for which I am thankful to Dr. Seok who has allowed me to work on his new XRD. My focus will be to improve the crystallinity of the films and find otpomized electrodeposition parameters.
I current have 2 conference proceedings publication, one peer-reviewed publication in journal of Nanomaterials, and one pending publication in IEEE Journal of Photovoltaics, I have already submitted the revised version and it is under review process.
I have participated in 14 conferences/meetings, I have given 6 oral presentations and 8 poster presentations. I have also attended and participated 2 workshops and 1 professional development seminar.