A Comprehensive Evaluation of Contact Recombination and Contact Resistivity Losses in Industrial Silicon Solar Cells

Reliable characterization techniques to accurately quantify the metallization-induced recombination losses as well as contact resistivity losses of screen-printed cells are crucial for successful optimization of the contact grid design. Previously, the dark saturation current density at the contact...

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Veröffentlicht in:IEEE journal of photovoltaics 2020-09, Vol.10 (5), p.1-6
Hauptverfasser: Li, Mengjie, Iqbal, Nafis, Yang, Zhihao, Lin, Xuli, Pannaci, Nicole Karam, Avalos, Christian, Shaw, Thomas, Jurca, Titel, Davis, Kristopher
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Sprache:eng
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Zusammenfassung:Reliable characterization techniques to accurately quantify the metallization-induced recombination losses as well as contact resistivity losses of screen-printed cells are crucial for successful optimization of the contact grid design. Previously, the dark saturation current density at the contact ( {J}_{\rm 0c} ) is often assumed to be constant for different finger width. Similarly, impact of finger width on contact resistivity ( {\rho }_{\rm c} ) is rarely reported. Therefore, we performed a comprehensive evaluation of  {J}_{\rm 0c} and {\rho }_{\rm c} as a function of finger width, spacing as well as firing temperature. We found out that {J}_{\rm 0c} increases from \approx 2000 to \approx 8100 \text{fA/cm}^{2} , when the finger width increases from 60 to 400 \mu m; and {\rho }_{\rm c} decrease from 7.2 to 2.2 \text{m}{\Omega }\cdot \text{cm}^{2} when using a wide-TLM rather than a narrow-TLM structure, for samples fired at 840  ^{\circ } C. Based on our cross-sectional and top-down scanning electron microscopy images, we believe that the physical root cause can be explained by the difference in the microstructure formed at the metal-silicon interface during the firing process for the screen-printed contacts.
ISSN:2156-3381
2156-3403
DOI:10.1109/JPHOTOV.2020.3003792