Investigation of polycrystalline silicon back surface field solar cells

1982 ◽  
Vol 29 (8) ◽  
pp. 1151-1155 ◽  
Author(s):  
W.A. Orr ◽  
M. Arienzo
Keyword(s):  
Solar Cells ◽  
Polycrystalline Silicon ◽  
Back Surface ◽  
Back Surface Field ◽  
Surface Field

Optimizing Back Surface Field of Heterojunction Thin-Film Solar Cells by Numerical Simulation

2011 ◽  
Vol 383-390 ◽  
pp. 267-271
Author(s):  
Gang Lu ◽  
Lu Zhang
Keyword(s):  
Solar Cells ◽  
Polycrystalline Silicon ◽  
Thin Film Solar Cells ◽  
Maximum Efficiency ◽  
Back Surface ◽  
Defect States ◽  
Back Surface Field ◽  
Heterojunction Solar Cells ◽  
Surface Field ◽  
Silicon Heterojunction Solar Cells

A new structure of amorphous/ polycrystalline silicon heterojunction solar cells is reported. For a-Si (n+)/poly-Si (p)/poly-Si(p+) structure, the concentration, thickness, and the defect states of BSF are discussed. It is shown that the cell performance improves with thickness between 10-15nm, concentration is of the order of 1E19cm-3, the maximum efficiency up to 20.45%.

scholarly journals Numerical Investigation of Graphene as a Back Surface Field Layer on the Performance of Cadmium Telluride Solar Cell

Molecules ◽  
2021 ◽  
Vol 26 (11) ◽  
pp. 3275
Author(s):  
Devendra KC ◽  
Deb Kumar Shah ◽  
M. Shaheer Akhtar ◽  
Mira Park ◽  
Chong Yeal Kim ◽  
...  
Keyword(s):  
Solar Cells ◽  
Solar Cell ◽  
Doping Concentration ◽  
Carrier Lifetime ◽  
Short Circuit ◽  
Back Surface ◽  
Back Surface Field ◽  
Cdte Solar Cell ◽  
Cdte Solar Cells ◽  
Surface Field

This paper numerically explores the possibility of ultrathin layering and high efficiency of graphene as a back surface field (BSF) based on a CdTe solar cell by Personal computer one-dimensional (PC1D) simulation. CdTe solar cells have been characterized and studied by varying the carrier lifetime, doping concentration, thickness, and bandgap of the graphene layer. With simulation results, the highest short-circuit current (Isc = 2.09 A), power conversion efficiency (h = 15%), and quantum efficiency (QE ~ 85%) were achieved at a carrier lifetime of 1 × 103 ms and a doping concentration of 1 × 1017 cm−3 of graphene as a BSF layer-based CdTe solar cell. The thickness of the graphene BSF layer (1 mm) was proven the ultrathin, optimal, and obtainable for the fabrication of high-performance CdTe solar cells, confirming the suitability of graphene material as a BSF. This simulation confirmed that a CdTe solar cell with the proposed graphene as the BSF layer might be highly efficient with optimized parameters for fabrication.

Screen-printed n-type Si solar cells with laser-doped selective back surface field

Solar Energy ◽  
2021 ◽  
Vol 220 ◽  
pp. 211-216
Author(s):  
H.P. Yin ◽  
W.S. Tang ◽  
J.B. Zhang ◽  
W. Shan ◽  
X.M. Huang ◽  
...  
Keyword(s):  
Solar Cells ◽  
Back Surface ◽  
Back Surface Field ◽  
Si Solar Cells ◽  
Surface Field ◽  
Screen Printed

Effects of buffer layer and back-surface field on MBE-grown InGaAsP/InGaAs solar cells

2016 ◽  
Vol 55 (2) ◽  
pp. 022301 ◽  
Author(s):  
Yuanyuan Wu ◽  
Lian Ji ◽  
Pai Dai ◽  
Ming Tan ◽  
Shulong Lu ◽  
...  
Keyword(s):  
Solar Cells ◽  
Buffer Layer ◽  
Back Surface ◽  
Back Surface Field ◽  
Surface Field

Numerical Study of TCO/Silicon Solar Cells with Novel Back Surface Field

2016 ◽  
Vol 45 (8) ◽  
pp. 3929-3934 ◽  
Author(s):  
M. Boumaour ◽  
S. Sali ◽  
A. Bahfir ◽  
S. Kermadi ◽  
L. Zougar ◽  
...  
Keyword(s):  
Solar Cells ◽  
Numerical Study ◽  
Silicon Solar Cells ◽  
Back Surface ◽  
Back Surface Field ◽  
Surface Field
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