CdS nanowire layers of enhanced transmittance for window layer applications in thin film solar cells

Author(s):  
Hongmei Dang ◽  
Suresh Rajaputra ◽  
Jianhao Chen ◽  
Sai Guduru ◽  
Nandu Reddy ◽  
...  
2013 ◽  
Vol 103 (7) ◽  
pp. 073903 ◽  
Author(s):  
Hyung Hwan Jung ◽  
Jung-Dae Kwon ◽  
Sunghun Lee ◽  
Chang Su Kim ◽  
Kee-Seok Nam ◽  
...  

Solar RRL ◽  
2019 ◽  
Vol 3 (10) ◽  
pp. 1900225 ◽  
Author(s):  
Liping Guo ◽  
Baiyu Zhang ◽  
Smriti Ranjit ◽  
Jacob Wall ◽  
Swapnil Saurav ◽  
...  

Energies ◽  
2019 ◽  
Vol 12 (6) ◽  
pp. 1123 ◽  
Author(s):  
Guanggen Zeng ◽  
Xia Hao ◽  
Shengqiang Ren ◽  
Lianghuan Feng ◽  
Qionghua Wang

The application of thinner cadmium sulfide (CdS) window layer is a feasible approach to improve the performance of cadmium telluride (CdTe) thin film solar cells. However, the reduction of compactness and continuity of thinner CdS always deteriorates the device performance. In this work, transparent Al2O3 films with different thicknesses, deposited by using atomic layer deposition (ALD), were utilized as buffer layers between the front electrode transparent conductive oxide (TCO) and CdS layers to solve this problem, and then, thin-film solar cells with a structure of TCO/Al2O3/CdS/CdTe/BC/Ni were fabricated. The characteristics of the ALD-Al2O3 films were studied by UV–visible transmittance spectrum, Raman spectroscopy, and atomic force microscopy (AFM). The light and dark J–V performances of solar cells were also measured by specific instrumentations. The transmittance measurement conducted on the TCO/Al2O3 films verified that the transmittance of TCO/Al2O3 were comparable to that of single TCO layer, meaning that no extra absorption loss occurred when Al2O3 buffer layers were introduced into cells. Furthermore, due to the advantages of the ALD method, the ALD-Al2O3 buffer layers formed an extremely continuous and uniform coverage on the substrates to effectively fill and block the tiny leakage channels in CdS/CdTe polycrystalline films and improve the characteristics of the interface between TCO and CdS. However, as the thickness of alumina increased, the negative effects of cells were gradually exposed, especially the increase of the series resistance (Rs) and the more serious “roll-over” phenomenon. Finally, the cell conversion efficiency (η) of more than 13.0% accompanied by optimized uniformity performances was successfully achieved corresponding to the 10 nm thick ALD-Al2O3 thin film.


2016 ◽  
Vol 2016 ◽  
pp. 1-8
Author(s):  
Pei-Ling Chen ◽  
Po-Wei Chen ◽  
Min-Wen Hsiao ◽  
Cheng-Hang Hsu ◽  
Chuang-Chuang Tsai

The enhancement of optical absorption of silicon thin-film solar cells by the p- and n-typeμc-SiOx:H as doped and functional layers was presented. The effects of deposition conditions and oxygen content on optical, electrical, and structural properties ofμc-SiOx:H films were also discussed. Regarding the dopedμc-SiOx:H films, the wide optical band gap (E04) of 2.33 eV while maintaining a high conductivity of 0.2 S/cm could be obtained with oxygen incorporation of 20 at.%. Compared to the conventionalμc-Si:H(p) as window layer inμc-Si:H single-junction solar cells, the application ofμc-SiOx:H(p) increased theVOCand led to a significant enhancement in the short-wavelength spectral response. Meanwhile, the employment ofμc-SiOx:H(n) instead of conventional ITO as back reflecting layer (BRL) enhanced the external quantum efficiency (EQE) ofμc-Si:H single-junction cell in the long-wavelength region, leading to a relative efficiency gain of 10%. Compared to the reference cell, the optimized a-Si:H/μc-Si:H tandem cell by applying p- and n-typeμc-SiOx:H films achieved aVOCof 1.37 V,JSCof 10.55 mA/cm2, FF of 73.67%, and efficiency of 10.51%, which was a relative enhancement of 16%.


2011 ◽  
Vol 1321 ◽  
Author(s):  
P. H. Cheng ◽  
S. W. Liang ◽  
Y. P. Lin ◽  
H. J. Hsu ◽  
C. H. Hsu ◽  
...  

ABSTRACTThe hydrogenated amorphous silicon (a-Si:H) single-junction thin-film solar cells were fabricated on SnO2:F-coated glasses by plasma-enhanced chemical vapor deposition (PECVD) system. The boron-doped amorphous silicon carbide (a-SiC:H) was served as the window layer (p-layer) and the undoped a-SiC:H was used as a buffer layer (b-layer). The optimization of the p/b/i/n thin-films in a-Si:H solar cells have been carried out and discussed. Considering the effects of light absorption, electron-hole extraction and light-induced degradation, the thicknesses of p, b, n and i layers have been optimized. The optimal a-Si:H thin-film solar cell having an efficiency of 9.46% was achieved, with VOC=906 mV, JSC=14.42 mA/cm2 and FF=72.36%.


Author(s):  
Md. Sharafat Hossain ◽  
Nowshad Amin ◽  
M. M. Aliyu ◽  
M. A. Matin ◽  
M. K. Siddiki ◽  
...  

2017 ◽  
Vol 214 (10) ◽  
pp. 1700132 ◽  
Author(s):  
X. Niu ◽  
H. Zhu ◽  
W. Zhang ◽  
X. Laing ◽  
Y. Guo ◽  
...  

Sign in / Sign up

Export Citation Format

Share Document