Hole-Collection Mechanism in Passivating Metal-Oxide Contacts on Si Solar Cells: Insights From Numerical Simulations

被引:71
|
作者
Vijayan, Ramachandran Ammapet [1 ]
Essig, Stephanie [2 ]
De Wolf, Stefaan [3 ]
Ramanathan, Bairava Ganesh [4 ]
Loeper, Philipp [2 ]
Ballif, Christophe [2 ]
Varadharajaperumal, Muthubalan [1 ]
机构
[1] SASTRA Deemed Univ, Sch Elect & Elect Engn, Device Modeling Lab, Thanjavur 613402, India
[2] Ecole Polytech Fed Lausanne, Inst Microengn, Photovolta & Thin Film Elect Lab, CH-2000 Neuchatel, Switzerland
[3] King Abdullah Univ Sci & Technol, KAUST Solar Ctr, Thuwal 239556900, Saudi Arabia
[4] Mundra Solar PV Ltd, Ahmadabad 370435, Gujarat, India
来源
IEEE JOURNAL OF PHOTOVOLTAICS | 2018年 / 8卷 / 02期
基金
瑞士国家科学基金会; 欧盟地平线“2020”; 欧洲研究理事会;
关键词
Hole collection; passivating contacts; silicon heterojunction (SHJ) solar cell; simulation; transition metal oxides; MOLYBDENUM; EFFICIENCY; LAYER; MOOX;
D O I
10.1109/JPHOTOV.2018.2796131
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
Silicon heterojunction solar cells enable high conversion efficiencies, thanks to their passivating contacts which consist of layered stacks of intrinsic and doped amorphous silicon. However, such contacts may reduce the photo current, when present on the illuminated side of the cell. This motivates the search for wider bandgap contacting materials, such as metal oxides. In this paper, we elucidate the precise impact of the material parameters of MoOx on device characteristics, based on numerical simulations. The simulation results allow us to propose design principles for hole-collecting induced junctions. We find that if MoOx has a sufficiently high electron affinity (>= 5.7 eV), direct band-to-band tunneling is the dominant transport mechanism; whereas if it has a lower electron affinity (< 5.7 eV), trap-assisted tunneling dominates, which might introduce additional series resistance. At even lower electron affinity, S-shaped J-V curves may appear for these solar cells, which are found to be due to an insufficient trap state density in the MoOx film in contrast to the expectation of better performance at low trap density. These traps may assist carrier transport when present near the conduction band edge of the MoOx film. Our simulations predict that performance optimization for the MoOx film has to target either 1) a high electron affinity and a moderate doping density film or, 2) if the electron affinity is lower than the optimum value, a high defect density not exceeding the doping density inside the film.
引用
收藏
页码:473 / 482
页数:10
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