Silicon Tunnel Junctions Produced by Ion Implantation and Diffusion Processes for Tandem Solar Cells

2018 ◽  
Vol 8 (6) ◽  
pp. 1436-1442
Author(s):  
Pierre Bellanger ◽  
Albert Minj ◽  
Alain Fave ◽  
Zakaria Djebbour ◽  
Stephane Roques ◽  
...  
Author(s):  
Shuai Zhou ◽  
Randy P. Tompkins ◽  
Kenneth A. Jones ◽  
Chad Gallinat ◽  
Paul Rotella ◽  
...  

Author(s):  
Savita Kashyap ◽  
Jaya Madan ◽  
Rahul Pandey ◽  
Rajnish Sharma

Abstract Achieved levels of Silicon-based passivated emitter and rear cell (PERC) solar cells' laboratory and module-level conversion efficiencies are still far from the theoretically achievable Auger limit of 29.4% for silicon solar cells, prominently due to emitter recombination and resistive losses. The emitter region in PERC devices is formed by using either ion implantation followed by a diffusion process or POCl3 diffusion. In ion-implanted emitter-based PERC, the process variables such as dose, energy, diffusion time, and temperature play a vital role in defining the characteristics of the emitter region. Detailed investigation of these parameters could provide a pathway to mitigate the recombination as well as resistive losses; however, it requires a considerable budget to optimize these parameters through a purely experimental approach. Therefore, advanced industrial standard process and device simulation are perceived in this work to carry out the comprehensive study of process variables. Investigation of ion implantation and diffusion process parameters on the PV performance of an upright pyramid textured, industrial standard stacked dielectric passivated PERC solar cell is carried out to deliver 22.8% conversion efficiency with improved PV parameters such as short circuit current density (JSC) of 40.8 mA/cm2, open-circuit voltage (VOC) of 686 mV, and fill-factor (FF) of 81.54% at optimized implantation and diffusion parameters, such as implantation dose of 5×1015 cm-2 with energy 30 keV followed 950 oC diffusion temperature and 30 min of diffusion time. The performance of the optimized PERC device is compared with already published large area screen printed contact-based device. This work may open up a window for the experimental work to understand the influence of process parameters on the emitter region to develop the highly efficient PERC solar cell in the future.


2015 ◽  
Vol 24 (10) ◽  
pp. 108802 ◽  
Author(s):  
Xin-He Zheng ◽  
San-Jie Liu ◽  
Yu Xia ◽  
Xing-Yuan Gan ◽  
Hai-Xiao Wang ◽  
...  

1983 ◽  
Vol 105 (4) ◽  
pp. 343-351 ◽  
Author(s):  
F.J. Bryant ◽  
A.K. Hariri ◽  
S. Salkalachen ◽  
C.G. Scott

2021 ◽  
Vol 11 (2) ◽  
pp. 408-414
Author(s):  
Daniel J. Chmielewski ◽  
Daniel L. Lepkowski ◽  
Jacob T. Boyer ◽  
Tyler J. Grassman ◽  
Steven A. Ringel

Author(s):  
Forrest Johnson ◽  
Sang Ho Song ◽  
Richard Liptak ◽  
Boris Chernomordik ◽  
Stephen A. Campbell

1991 ◽  
Vol 219 ◽  
Author(s):  
K. Prasad ◽  
U. Kroll ◽  
F. Finger ◽  
A. Shah ◽  
J-L. Dorter ◽  
...  

ABSTRACTWe have investigated the influence of substrate temperature on the optoelectronic and structural properties of heavily doped μc-Si:H, prepared with the Very High Frequency Glow Discharge process. At substrate temperatures as low as 160°C we obtain, for films with 0.5μm thickness, maximum conductivities of 100 S/cm and 20 S/cm for <n> and <p> material, respectively. Starting from these values the deposition parameters were optimised for ultrathin layers having thicknesses in the range of 100 to 500Å. We observe that boron doping plays a critical role in the crystallisation of ultrathin films. The thinnest layers investigated so far show conductivities of 0.2 S/cm at d=100Å for <n>, and 0.2 S/cm at d=250Å for <p> material. These properties make μc-Si:H films attractive candidates to form tunnel junctions in tandem solar cells.


2011 ◽  
Vol 20 (7) ◽  
pp. 078402 ◽  
Author(s):  
Wen-Jie Yao ◽  
Xiang-Bo Zeng ◽  
Wen-Bo Peng ◽  
Shi-Yong Liu ◽  
Xiao-Bing Xie ◽  
...  

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