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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


  1. EEE23 Low Cost and High Efficiency Si/TMO Heterojunction Solar cell Loh Zhang Chao, Xavier | Lim Hua En Dr Rusli | Dr Ari Bimo Prakoso

  2. 1. Rationale behind our research Why we decided to embark on this research

  3. 3 Traditional Solar Cells Rationale ○ High Temperature - during doping of P- type and N-type Si junctions ○ High Costs ○ High Payback Time of > 6 years

  4. 4 Unfavourable for widespread application

  5. Background of our Research Transition Metal Oxides such as MoO 3 , V 2 O 5 & Cu 2 O 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

  6. “ 6 Research Goal - To identify which TMO is the best out of the three to spearhead future research into TMO/nSI Solar Cell research

  7. “ 7 Methodology Fabrication of Sample Compare results Deposition Shadow of layers Wafer Cleaning of Characterisatio Mask -Back Cutting Samples n of Solar Cell -Silver Contact Contact -TMO -ITO

  8. 8 Structure of our Solar Cell

  9. Some Equipment Used for Fabrication / Characterisation Electron Beam Evaporation | Radio Frequency Sputtering | Solar Simulator & Machine Machine Keithley Sourcemeter

  10. Deposition of Deposition of Obtaining Photovoltaic - Back Contact - TMO - ITO Parameters to compare - Silver Contacts with Shadow between solar cells Mask Electron Beam Evaporation | Radio Frequency Sputtering | Solar Simulator & Machine Machine Keithley Sourcemeter

  11. Specifics on how we used the equipment Power intensity set at 1. 100mW/cm 2 with fixed Sample Size of 1 cm 2 2. 2 Probe Method for more realistic results Solar Simulator & Keithley Sourcemeter

  12. 3. Characterisation of samples Values obtained from characterisation and analysis

  13. - Short Circuit Current 4 different PV density (Jsc) parameters measured - Open Circuit Voltage (Voc) - Fill factor (FF) - Efficiency (PCE)

  14. Short Circuit - Measures current Current Density at 0V (Jsc) - Dependent on light absorption of solar cell and carriers generated and collected

  15. - Measures voltage at 0A Open Circuit - Dependent on Voltage (Voc) saturation current, which depends on recombination of carriers

  16. - Measures the ratio of maximum power Maximum Fill Factor (FF) Power to Isc x Voc - Allows us to determine the amount of series, shunt resistance in the cell

  17. - The ratio of output to input power, Efficiency calculated through (PCE) Pmax/Pin - The main point of comparison between different solar cells

  18. Results Data and Analysis

  19. 19 Jsc/ mA cm - Structure Voc/V FF/% PCE/% 2 Results Collected 27.8 0.570 59.8 9.5 MoO3 26.7 0.568 57.0 8.6 V2O5 30.1 0.261 37.3 2.9 Cu2O Without 14.8 0.054 24.3 0.2 TMO

  20. - Comparable Struct values for all 3 Jsc/ mA Analysis - Jsc Voc/V FF/% PCE/% ure cm -2 - Cu 2 O has a slightly 27.8 0.570 59.8 9.5 MoO3 higher Jsc value, 26.7 0.568 57.0 8.6 V2O5 which could be due to higher 30.1 0.261 37.3 2.9 Cu2O capability in Withou 14.8 0.054 24.3 0.2 t TMO photon carrier generation

  21. - MoO 3 has highest Struct Voc value, Jsc/ mA Analysis - Voc Voc/V FF/% PCE/% ure cm -2 suggesting lowest 27.8 0.570 59.8 9.5 rate of MoO3 recombination 26.7 0.568 57.0 8.6 V2O5 - Cu 2 O’s low Voc 30.1 0.261 37.3 2.9 Cu2O value may be due Withou 14.8 0.054 24.3 0.2 to higher t TMO recombination current in the cell

  22. - MoO 3 also has a Struct high FF, which Jsc/ mA Analysis - FF Voc/V FF/% PCE/% ure cm -2 suggests the solar 27.8 0.570 59.8 9.5 cell has very little MoO3 series 26.7 0.568 57.0 8.6 V2O5 resistance/more 30.1 0.261 37.3 2.9 Cu2O shunt resistance Withou 14.8 0.054 24.3 0.2 - Cu 2 O’s lower FF t TMO could be due to higher series resistance in cell

  23. - MoO 3 has the Struct highest PCE value Jsc/ mA Analysis - PCE Voc/V FF/% PCE/% ure cm -2 of 9.5%, showing 27.8 0.570 59.8 9.5 its potential MoO3 26.7 0.568 57.0 8.6 V2O5 - Cu 2 O’s lower PCE 30.1 0.261 37.3 2.9 value of 2.8% was Cu2O mainly due to the Withou 14.8 0.054 24.3 0.2 t TMO lower Voc and FF values hindering max power

  24. 4. Conclusion Summary of Analysis and areas for further research

  25. - About 20% reduction in cost Conclusion - MoO 3 achieved the best Voc, FF and PCE values, highlighting its favourable properties for use - Despite relatively lower PCE values, MoO 3 displays potential for future research and large improvements

  26. - Vary thickness of ITO Areas for and TMO layers to better optimise solar future cell research - Use single wavelength analysis to better analyse the structure of the solar cell, absorption probabilities at different sections - Utilise alternative fabrication methods like spin coating

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