Optoelectronic characteristics of a-SiC:H-based pin thin film LEDs having a thin Mo buffer layer in contact with p-type a-Si:H

1998 ◽  
Vol 34 (14) ◽  
pp. 1433 ◽  
Author(s):  
Yen-Ann Chen ◽  
Yung-Hung Wu ◽  
Wen-Chin Tsay ◽  
Li-Hong Laih ◽  
Jyh-Wong Hong ◽  
...  
Keyword(s):  
Type A ◽  
2010 ◽  
Vol 94 (12) ◽  
pp. 2332-2336 ◽  
Author(s):  
Sun-Young Park ◽  
Hye-Ri Kim ◽  
Yong-Jin Kang ◽  
Dong-Ho Kim ◽  
Jae-Wook Kang

2011 ◽  
Vol 3 ◽  
pp. 51-57 ◽  
Author(s):  
G. Cannella ◽  
F. Principato ◽  
M. Foti ◽  
C. Garozzo ◽  
S. Lombardo
Keyword(s):  
Type A ◽  

Coatings ◽  
2021 ◽  
Vol 11 (1) ◽  
pp. 52
Author(s):  
Asmaa Soheil Najm ◽  
Puvaneswaran Chelvanathan ◽  
Sieh Kiong Tiong ◽  
Mohammad Tanvirul Ferdaous ◽  
Seyed Ahmad Shahahmadi ◽  
...  

A CdS thin film buffer layer has been widely used as conventional n-type heterojunction partner both in established and emerging thin film photovoltaic devices. In this study, we perform numerical simulation to elucidate the influence of electrical properties of the CdS buffer layer, essentially in terms of carrier mobility and carrier concentration on the performance of SLG/Mo/p-Absorber/n-CdS/n-ZnO/Ag configured thin film photovoltaic devices, by using the Solar Cell Capacitance Simulator (SCAPS-1D). A wide range of p-type absorber layers with a band gap from 0.9 to 1.7 eV and electron affinity from 3.7 to 4.7 eV have been considered in this simulation study. For an ideal absorber layer (no defect), the carrier mobility and carrier concentration of CdS buffer layer do not significantly alter the maximum attainable efficiency. Generally, it was revealed that for an absorber layer with a conduction band offset (CBO) that is more than 0.3 eV, Jsc is strongly dependent on the carrier mobility and carrier concentration of the CdS buffer layer, whereas Voc is predominantly dependent on the back contact barrier height. However, as the bulk defect density of the absorber layer is increased from 1014 to 1018 cm−3, a CdS buffer layer with higher carrier mobility and carrier concentration is an imperative requirement to a yield device with higher conversion efficiency and a larger band gap-CBO window for realization of a functional device. Most tellingly, simulation outcomes from this study reveal that electrical properties of the CdS buffer layer play a decisive role in determining the progress of emerging p-type photo-absorber layer materials, particularly during the embryonic device development stage.


2020 ◽  
Vol 8 (2) ◽  
pp. 567-580
Author(s):  
Calvin J. Lee ◽  
Fadi M. Jradi ◽  
Valerie D. Mitchell ◽  
Jonathan White ◽  
Christopher R. McNeill ◽  
...  

Structure–property studies of p-type oligothiophene-based materials linking sidechain substituents, photovoltaic performance and thin-film morphology leading to key design guidelines.


2015 ◽  
Vol 1771 ◽  
pp. 3-8 ◽  
Author(s):  
Xiaodan Zhang ◽  
Bofei Liu ◽  
Lisha Bai ◽  
Fang jia ◽  
Shuo Wang ◽  
...  

ABSTRACTThe unique properties of silicon oxide materials, no matter intrinsic or doped, utilized in thin film solar cells (TFSCs) in the area of photovoltaic (PV) are making TFSCs one of the most attractive photovoltaic technologies for the development of high-performing electricity production units to be integrated in everyday life. In comparison to other silicon materials, the particular diphasic structure of silicon oxide materials, in which hydrogenated microcrystalline silicon (μc-Si:H) crystallites are surrounded by an oxygen-rich hydrogenated amorphous silicon (a-Si:H) phase, causes them present excellent photoelectrical material properties, such as a low-parasitic absorption in the broadband spectral range, independent controllability of longitudinal and lateral conductivity, refractive indices (3.5-2.0), band gap (2.0-2.6 eV) and conductivity tenability (with orders of 1-10-9 S/cm) with oxygen doping, and so on. Various types of silicon oxide materials, including intrinsic, p- or n- type, further applied in TFSCs have also played significant roles in improving the efficiency of various types of single-, dual-, and triple-junction thin-film solar cells from both the optical and electrical points of view. In this paper, we present our latest progress in studying the performance improvement role of intrinsic or doped silicon oxide materials in pin-type a-Si:H, a-SiGe:H, and μc-Si:H single-junction solar cells. By effectively tuning the band gap values of intrinsic a-SiOx:H materials with oxygen doping and adopting the layers with a suitable band gap (1.86 eV) as the P/I buffer layers of a-Si:H solar cells fabricated on metal organic chemical vapor deposition (MOCVD) boron-doped zinc oxide (ZnO:B) substrates, a significant Voc increases up to 909 mV and an excellent external quantum efficiency (EQE) response of 75% at the 400 nm typical wavelength can be achieved by matching the band gap discontinuity between the p-type nc-SiOx:H window and a-Si:H intrinsic layers. The serious leakage current characteristics of pin-type narrow-gap (Eg<1.5 eV) a-SiGe:H single-junction solar cells can also be finely tuned by integrating an n-type μc-SiOx:H layer with a small oxygen content in addition to improving the long-wavelength response, an effective approach gives rise to the highest FF of 70.62% for pin-type a-SiGe:H single-junction solar cells with an average band gap of 1.48 eV. In addition, our studies proved that the application of p-type μc-SiOx:H window layers in μc-Si:H single-junction solar cells can effectively improve the short-wavelength light coupling by suppressing the parasitic absorption and promoting the anti-reflectivity with a graded refractive index profile. On the basis of the optimum single-junction solar cells with omnipotent silicon oxide materials, an initial efficiency of 16.07% has been achieved for pin-type a-Si:H/a-SiGe:H/μc-Si:H triple-junction solar cells with an active area of 0.25 cm2. The omnipotent properties of silicon oxide layers in TFSCs, including effective optical coupling and trapping, suitability in compensating for the band gap discontinuity, the shunt-quenching capacity, and so on, make them likely to be extended to other types of solar cells such as polycrystalline chalcopyrite Cu(In,Ga)Se2 (CIGS) and perovskite-sensitized solar cells, opening up new opportunities for acquiring solar cells with higher performance.


2015 ◽  
Vol 3 (30) ◽  
pp. 15583-15590 ◽  
Author(s):  
Bofei Liu ◽  
Zhonghua Jin ◽  
Lisha Bai ◽  
Junhui Liang ◽  
Qixing Zhang ◽  
...  

A catalyst-free and stable p-type a-SiC:H protected a-Si/a-SiGe tandem photocathode with high photovoltage is demonstrated for efficient solar water splitting.


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