scholarly journals Inline deposited PassDop layers for rear side passivation and contacting of p-type c-Si PERL solar cells with high bifaciality

Author(s):  
Mohammad Hassan Norouzi ◽  
Pierre Saint-Cast ◽  
Elmar Lohmüller ◽  
Sabrina Lohmüller ◽  
Bernd Steinhauser ◽  
...  
Keyword(s):  
Type C ◽  
2012 ◽  
Vol 106 ◽  
pp. 80-83 ◽  
Author(s):  
Pablo Ortega ◽  
Isidro Martín ◽  
Gema Lopez ◽  
Monica Colina ◽  
Albert Orpella ◽  
...  

Author(s):  
Quanyuan Shang ◽  
Walter Seaman ◽  
Mike Whitney ◽  
Mark George ◽  
John Madocks ◽  
...  

2019 ◽  
Vol 200 ◽  
pp. 109937 ◽  
Author(s):  
Paul Procel ◽  
Philipp Löper ◽  
Felice Crupi ◽  
Christophe Ballif ◽  
Andrea Ingenito

2006 ◽  
Vol 352 (9-20) ◽  
pp. 1972-1975 ◽  
Author(s):  
Ying Xu ◽  
Zhihua Hu ◽  
Hongwei Diao ◽  
Yi Cai ◽  
Shibin Zhang ◽  
...  

2012 ◽  
Vol 195 ◽  
pp. 310-313 ◽  
Author(s):  
Abdelazize Laades ◽  
Heike Angermann ◽  
Hans Peter Sperlich ◽  
Uta Stürzebecher ◽  
Carlos Alberto Díaz Álvarez ◽  
...  

Aluminum oxide (AlOx) is currently under intensive investigation for use in surface passivation schemes in solar cells. AlOx films contain negative charges and therefore generate an accumulation layer on p-type silicon surfaces, which is very favorable for the rear side of p-type silicon solar cells as well as the p+-emitter at the front side of n-type silicon solar cells. However, it has been reported that quality of an interfacial silicon sub-oxide layer (SiOx), which is usually observed during deposition of AlOx on Silicon, strongly impacts the silicon/AlOx interface passivation properties [1]. The present work demonstrates that a convenient way to control the interface is to form thin wet chemical oxides of high quality prior to the deposition of AlOx/a-SiNx:H stacks by the plasma enhanced chemical vapor deposition (PECVD).


1999 ◽  
Vol 557 ◽  
Author(s):  
Bolko Von Roedern ◽  
Gottfried H. Bauer

AbstractThis paper discusses material requirements for junction layers needed to obtain solar cells with highest possible open-circuit voltages (VOC). In a typical a-Si:H-based “p/i/n” solar cell, this includes the transparent conductive oxide (TCO) contact layer, the p-layer, a “buffer layer” inserted at the p/i interface, and the surface portion of the intrinsic layer. In HIT-cells, the i-layer between (n-type) c-Si and (p-type) a-Si:H may be regarded as the buffer. Our suggestion to obtain high values of VOC relies on using materials with high lifetimes and low carrier mobilities that are capable of reducing surface or junction recombination by reducing the flow of carriers into this loss-pathway. We provide a general calculation that supports these approaches and can explain why these schemes are beneficial for all solar cells.


2021 ◽  
Vol 219 ◽  
pp. 110809
Author(s):  
Andrea Ingenito ◽  
Sofia Libraro ◽  
Philippe Wyss ◽  
Christophe Allebé ◽  
Matthieu Despeisse ◽  
...  

2019 ◽  
Vol 966 ◽  
pp. 409-414
Author(s):  
Dadan Hamdani ◽  
Yoyok Cahyono ◽  
Gatut Yudoyono ◽  
Darminto

Using well-practiced AFORS-HET software, thin film a-Si:H Bifacial Solar Cells (BFSCs) has been investigated and simulated. The aim of this study is to simulate performances of a-Si:H BFCs with structure of Glass/TCO/(n) a-Si:H/(i) a-Si:H/(p) a-Si:H/TCO/Glass. The results show that the optimized band gap for each layers are 2.0 eV (n-type), 1.7 eV (i-type) and 2.0 eV (p-type), respectively. The final simulation show that a significant increase VOC, JSC, FF and Eff for both side of a-Si:H BFSCs. Finally, the maximum efficiency obtained are 7.79% for the front side and 5.68% for the rear side, respectively.


2020 ◽  
Vol 10 (2) ◽  
pp. 407-416 ◽  
Author(s):  
Supawan Joonwichien ◽  
Masaaki Moriya ◽  
Satoshi Utsunomiya ◽  
Yasuhiro Kida ◽  
Katsuhiko Shirasawa ◽  
...  
Keyword(s):  
P Type ◽  

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