Performance improvements of organic solar cell using dual cathode buffer layers

2018 ◽  
Vol 18 (12) ◽  
pp. 1592-1599 ◽  
Author(s):  
Sheenam Sachdeva ◽  
Jagdish Kaur ◽  
Kriti Sharma ◽  
S.K. Tripathi
RSC Advances ◽  
2014 ◽  
Vol 4 (13) ◽  
pp. 6646 ◽  
Author(s):  
Zhenhua Lin ◽  
Jingjing Chang ◽  
Changyun Jiang ◽  
Jie Zhang ◽  
Jishan Wu ◽  
...  

2011 ◽  
Vol 95 (12) ◽  
pp. 3460-3464 ◽  
Author(s):  
Chien-Jung Huang ◽  
Jhong-Ciao Ke ◽  
Wen-Ray Chen ◽  
Teen-Hang Meen ◽  
Cheng-Fu Yang

2020 ◽  
Vol 16 ◽  
Author(s):  
Minh Duc Tran ◽  
Nguyen Dinh Lam

Background: The active layer not only must have a strong light absorption in the visible spectrum, but must also be sufficient for charge carrier transport to the electrodes. Electrons in conducting polymer transport by hopping between different energy levels, resulted in much lower charge mobility. Therefore, the thickness of active layer must be limited so the separated charge can reach the corresponding electrodes without recombination. However, thin active layer has weaker light absorption, resulting in the low photogenerated current in organic solar cell devices. Furthermore, buffer layers usually have high charge mobility, which in turn would enhance the transportation of charge from the active layer to electrodes. Metal oxides have been studied to be used as cathode buffer layer such as titanium dioxide (TiO2), zinc oxide (ZnO), etc. Objective: In this work, behaviors of the photon-electrical characteristics with variation in thickness of the active (poly(3-hexylthiophene-2,5-diyl) and phenyl-C61 butyric acid methyl ester blend) and buffer (zinc oxide) layers were investigated. Method: The influences of the thickness of the active and buffer layers on characteristic parameters of organic solar cells were investigated by solving the drift and diffusion equation with the photogenerated current given by Hetch equation. Results: The optimum thickness was obtained around 100 nm and below 10 nm for the active and the ZnO buffer layers, respectively. Conclusion: Thinner active layer resulted in lower photocurrent due to poor light absorption while at 150 nm thick and above, PCE of the device reduced rapidly because of high recombination rate of photogenerated electron-hole pairs. ZnO buffer layer was used as an electron transport layer and a hole blocking layer in order to improve the cell’s performance. The addition of ZnO enhanced the PCE up to 2.48 times higher than conventional device.


2015 ◽  
Vol 26 (12) ◽  
pp. 9891-9897 ◽  
Author(s):  
Godfrey Keru ◽  
Patrick G. Ndungu ◽  
Vincent O. Nyamori ◽  
Genene T. Mola

2019 ◽  
Author(s):  
Matthew Morgan ◽  
Maryam Nazari ◽  
Thomas Pickl ◽  
J. Mikko Rautiainen ◽  
Heikki M. Tuononen ◽  
...  

The electrophilic borylation of 2,5-diarylpyrazines results in the formation of boron-nitrogen doped dihydroindeno[1,2-<i>b</i>]fluorene which can be synthesized via mildly air-sensitive techniques and the end products handled readily under atmosphereic conditions. Through transmetallation via diarylzinc reagents a series of derivatives were sythesized which show broad absorption profiles that highlight the versatility of this backbone to be used in organic solar cell devices. These compounds can be synthesized in large yields, in alow number of steps and functionalized at many stages along the way providing a large depth of possibilities. Exploratory device paramaters were studied and show PCE of 2%.


2017 ◽  
Vol 7 (2) ◽  
pp. 37
Author(s):  
Dhuriya Deepti ◽  
Kumar Brijesh ◽  
Chauhan R.K. ◽  
◽  
◽  
...  

2020 ◽  
Vol 16 (4) ◽  
pp. 556-567
Author(s):  
Asma Khalil ◽  
Zubair Ahmad ◽  
Farid Touati ◽  
Mohamed Masmoudi

Background: The photo-absorption and light trapping through the different layers of the organic solar cell structures are a growing concern now-a-days as it affects dramatically the overall efficiency of the cells. In fact, selecting the right material combination is a key factor in increasing the efficiency in the layers. In addition to good absorption properties, insertion of nanostructures has been proved in recent researches to affect significantly the light trapping inside the organic solar cell. All these factors are determined to expand the absorption spectrum and tailor it to a wider spectrum. Objective: The purpose of this investigation is to explore the consequence of the incorporation of the Ag nanostructures, with different sizes and structures, on the photo absorption of the organic BHJ thin films. Methods: Through a three-dimensional Maxwell solver software, Lumerical FDTD, a simulation and comparison of the optical absorption of the three famous organic materials blends poly(3- hexylthiophene): phenyl C71 butyric acid methyl ester (P3HT:PCBM), poly[N-9″-heptadecanyl-2,7- carbazole-alt-5,5-(4′,7′-di-2-thienyl-2′,1′,3′-benzothiadiazole)]: phenyl C71 butyric acid methyl ester (PCDTBT:PCBM) and poly[2,6-(4,4-bis-(2-ethylhexyl)-4H-cyclopenta[2,1-b;3,4-b′]dithiophene)-alt- 4,7-(2,1,3-benzothiadiazole)]: phenyl C71 butyric acid methyl ester (PCDPDTBT:PCBM) has been conducted. Furthermore, FDTD simulation study of the incorporation of nanoparticles structures with different sizes, in different locations and concentrations through a bulk heterojunction organic solar cell structure has also been performed. Results: It has been demonstrated that embedding nanostructures in different locations of the cell, specifically in the active layer and the hole transporting layer had a considerable effect of widening the absorption spectrum and increasing the short circuit current. The effect of incorporation the nanostructures in the active layer has been proved to be greater than in the HTL. Furthermore, the comparison results showed that, PCDTBT:PCBM is no more advantageous over P3HT:PCBM and PCPDTBT:PCBM, and P3HT:PCBM took the lead and showed better performance in terms of absorption spectrum and short circuit current value. Conclusion: This work revealed the significant effect of size, location and concentration of the Ag nanostructures while incorporated in the organic solar cell. In fact, embedding nanostructures in the solar cell widen the absorption spectrum and increases the short circuit current, this result has been proven to be significant only when the nanostructures are inserted in the active layer following specific dimensions and structures.


2021 ◽  
Vol 543 ◽  
pp. 148863
Author(s):  
Dhanasekaran Vikraman ◽  
Hailiang Liu ◽  
Sajjad Hussain ◽  
K. Karuppasamy ◽  
Hae-Kyung Youi ◽  
...  

2021 ◽  
pp. 2102361
Author(s):  
Shucheng Qin ◽  
Zhenrong Jia ◽  
Lei Meng ◽  
Can Zhu ◽  
Wenbin Lai ◽  
...  

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