Effects of dielectric structure of HfO2 on carrier generation rate in Si substrate and channel mobility

2004 ◽  
Vol 84 (12) ◽  
pp. 2148-2150 ◽  
Author(s):  
Chang Yong Kang ◽  
Hag-Ju Cho ◽  
Rino Choi ◽  
Chang Seok Kang ◽  
Young Hee Kim ◽  
...  
2011 ◽  
Vol 99 (5) ◽  
pp. 053126 ◽  
Author(s):  
W. D. A. M. de Boer ◽  
M. T. Trinh ◽  
D. Timmerman ◽  
J. M. Schins ◽  
L. D. A. Siebbeles ◽  
...  

2020 ◽  
Vol 31 (05) ◽  
pp. 2050076
Author(s):  
M. Ismail Fathima ◽  
K. S. Joseph Wilson

Carrier generation is one of the important processes in solar cell operations. The generation rate depends on the number of photons absorbed by solar cell. This absorption of photons is affected by the reflection losses. The light trapping technique is used to minimize the reflection loss. In this work, a theoretical design of Effective Interface Antireflective Coating (EI-ARC) in solar cell is proposed which is based on the theory of Fabry–Perot interference filters. This design is composed of a space index layer with two subsystems of multilayer, which allows multiple reflections within it. It is shown that the combination of this two systems yields high transmission values over a narrow spectral range. This EI-ARC model increases the Internal Quantum Efficiency (IQE) and carrier generation rate of solar cell. These parameters are significant to raise the efficiency of the solar cell.


1990 ◽  
Vol 192 ◽  
Author(s):  
H. R. Park ◽  
J. Z. Liu ◽  
P. Roca i Cabarrocas ◽  
A. Maruyama ◽  
M. Isomura ◽  
...  

ABSTRACTUsing a Kr ion laser (λ = 647.1 nm) to produce a carrier generation rate G of 3 × 1020 cm−3s−1, we have saturated the light-induced defect generation in hydrogenated (and fluorinated) amorphous silicon (a-Si:H(F)), within a few hours near room temperature. While the defect generation rate scales roughly with 1/G2, the saturation defect densities Ns,sat are essentially independent of G. The saturation is not due to thermal annealing. We have further measured Ns,sat m 37 a-Si:H(F) films grown in six different reactors under different conditions. The results show that Ns,sat lies between 5 × 1016 and 2 × 1017 cm−3, that Ns,sat drops with decreasing optical gap and hydrogen content, and that Ns,sat is not correlated with the initial defect density or with the Urbach energy.


1985 ◽  
Vol 28 (12) ◽  
pp. 1241-1243 ◽  
Author(s):  
Jože Furlan ◽  
Slavko Amon

1991 ◽  
Vol 30 (Part 1, No. 1) ◽  
pp. 31-32 ◽  
Author(s):  
Kazuhiro Sasaki ◽  
Kazunori Sato

Plasmonics ◽  
2019 ◽  
Vol 14 (6) ◽  
pp. 1711-1716
Author(s):  
Iraj S. Amiri ◽  
Hossein Mohammadi

1970 ◽  
Vol 13 (12) ◽  
pp. 1519-1526 ◽  
Author(s):  
J.L. Prince ◽  
J.J. Wortman ◽  
L.K. Monteith ◽  
J.R. Hauser

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