EEE23
Low Cost and High Efficiency Si/TMO Heterojunction Solar cell
Loh Zhang Chao, Xavier | Lim Hua En Dr Rusli | Dr Ari Bimo Prakoso
EEE23 Low Cost and High Efficiency Si/TMO Heterojunction Solar cell - - PowerPoint PPT Presentation
EEE23 Low Cost and High Efficiency Si/TMO Heterojunction Solar cell Loh Zhang Chao, Xavier | Lim Hua En Dr Rusli | Dr Ari Bimo Prakoso 1. Rationale behind our research Why we decided to embark on this research 3 Traditional Solar Cells
EEE23
Low Cost and High Efficiency Si/TMO Heterojunction Solar cell
Loh Zhang Chao, Xavier | Lim Hua En Dr Rusli | Dr Ari Bimo Prakoso
1. Rationale behind
Why we decided to embark
Rationale
○ High Temperature
type and N-type Si junctions
3
○ High Costs ○ High Payback Time
Traditional Solar Cells
Unfavourable for widespread application
4
Background of our Research
Transition Metal Oxides such as MoO3, V2O5 & Cu2O have shown favourable properties as P-type Si junction replacements ➢ High Work Functions that help form strong electronic barrier with nSi ➢ Lower Temperature of production ➢ Lower Cost that allows greater deployment ➢ More stable than other organic polymer material
Research Goal
three to spearhead future research into TMO/nSI Solar Cell research
6
Methodology
7
Wafer Cutting Cleaning of Samples Characterisatio n of Solar Cell Shadow Mask
Contact
Deposition
Contact
Fabrication of Sample Compare results
8
Structure of our Solar Cell
Some Equipment Used for Fabrication / Characterisation
Electron Beam Evaporation | Radio Frequency Sputtering | Solar Simulator & Machine Machine Keithley Sourcemeter
Electron Beam Evaporation | Radio Frequency Sputtering | Solar Simulator & Machine Machine Keithley Sourcemeter Deposition of
Mask Deposition of
Obtaining Photovoltaic Parameters to compare between solar cells
Specifics on how we used the equipment
Solar Simulator & Keithley Sourcemeter 2 Probe Method for more realistic results Power intensity set at 100mW/cm2 with fixed Sample Size of 1 cm2 1. 2.
3. Characterisation
Values obtained from characterisation and analysis
4 different PV parameters measured
density (Jsc)
(Voc)
Short Circuit Current Density (Jsc)
at 0V
light absorption
carriers generated and collected
Open Circuit Voltage (Voc)
voltage at 0A
saturation current, which depends on recombination
Fill Factor (FF)
to Isc x Voc
determine the amount of series, shunt resistance in the cell
Maximum Power
Efficiency (PCE)
to input power, calculated through Pmax/Pin
comparison between different solar cells
Results
Data and Analysis
Results Collected
Structure
Jsc/ mA cm-
2Voc/V FF/% PCE/% MoO3
27.8 0.570 59.8 9.5
V2O5
26.7 0.568 57.0 8.6
Cu2O
30.1 0.261 37.3 2.9
Without TMO
14.8 0.054 24.3 0.2
19
Analysis - Jsc
values for all 3
Struct ure
Jsc/ mA cm-2 Voc/V FF/% PCE/% MoO3
27.8 0.570 59.8 9.5
V2O5
26.7 0.568 57.0 8.6
Cu2O
30.1 0.261 37.3 2.9
Withou t TMO
14.8 0.054 24.3 0.2
higher Jsc value, which could be due to higher capability in photon carrier generation
Analysis - Voc
Voc value, suggesting lowest rate of recombination
Struct ure
Jsc/ mA cm-2 Voc/V FF/% PCE/% MoO3
27.8 0.570 59.8 9.5
V2O5
26.7 0.568 57.0 8.6
Cu2O
30.1 0.261 37.3 2.9
Withou t TMO
14.8 0.054 24.3 0.2
value may be due to higher recombination current in the cell
Analysis - FF
high FF, which suggests the solar cell has very little series resistance/more shunt resistance
Struct ure
Jsc/ mA cm-2 Voc/V FF/% PCE/% MoO3
27.8 0.570 59.8 9.5
V2O5
26.7 0.568 57.0 8.6
Cu2O
30.1 0.261 37.3 2.9
Withou t TMO
14.8 0.054 24.3 0.2
could be due to higher series resistance in cell
Analysis - PCE
highest PCE value
its potential
Struct ure
Jsc/ mA cm-2 Voc/V FF/% PCE/% MoO3
27.8 0.570 59.8 9.5
V2O5
26.7 0.568 57.0 8.6
Cu2O
30.1 0.261 37.3 2.9
Withou t TMO
14.8 0.054 24.3 0.2
value of 2.8% was mainly due to the lower Voc and FF values hindering max power
4. Conclusion
Summary of Analysis and areas for further research
Conclusion
cost
Voc, FF and PCE values, highlighting its favourable properties for use
PCE values, MoO3 displays potential for future research and large improvements
Areas for future research
and TMO layers to better optimise solar cell
analysis to better analyse the structure of the solar cell, absorption probabilities at different sections
fabrication methods like spin coating