Understanding the impact of side-chains on photovoltaic performance in efficient all-polymer solar cells

2019 ◽  
Vol 7 (40) ◽  
pp. 12641-12649 ◽  
Author(s):  
Bin Li ◽  
Qilin Zhang ◽  
Gaole Dai ◽  
Hua Fan ◽  
Xin Yuan ◽  
...  

We performed side-chain fluorination and alkylthio substituent in a template conjugated polymer and further investigate their impact on polymer–polymer solar cell performance.

RSC Advances ◽  
2020 ◽  
Vol 10 (63) ◽  
pp. 38344-38350
Author(s):  
Kai Wang ◽  
Sheng Dong ◽  
Xudong Chen ◽  
Ping Zhou ◽  
Kai Zhang ◽  
...  

Ternary all-polymer solar cells are fabricated using an N2200 acceptor and two donor polymers (PF2 and PM2) with complementary absorption.


2017 ◽  
Vol 8 (2) ◽  
pp. 1701552 ◽  
Author(s):  
Tadanori Kurosawa ◽  
Xiaodan Gu ◽  
Kevin L. Gu ◽  
Yan Zhou ◽  
Hongping Yan ◽  
...  

2018 ◽  
Vol 271 ◽  
pp. 106-111
Author(s):  
Jun Ning ◽  
Ming Ming Bao ◽  
Lian Hong ◽  
Hasichaolu ◽  
Bolag Altan ◽  
...  

Research on polymer solar cells has attracted increasing attention in the past few decades due to the advantages such as low cost of fabrication, ease of processing, mechanical flexibility, etc. In recent years, non-fullerene polymer solar cells are extensively studied, because of the reduced voltage losses, and the tunability of absorption spectra and molecular energy level of non-fullerene acceptors. In this work, polymer solar cells based on conjugated polymer (PBDB-T: poly [(2,6-(4,8-bis (5-(2-ethylhexyl) thiophen-2-yl)-benzo [1,2-b:4,5-b’] dithiophene))-alt-(5,5-(1’,3’-di-2-thienyl-5’,7’-bis (2-ethylhexyl) benzo [1’,2’-c:4’,5’-c’] dithiophene-4,8-dione))]) and non-fullerene electron acceptor (ITIC: 3,9-bis (2-methylene-(3-(1,1-dicyanomethylene)-indanone)) -5,5,11,11-tetrakis (4-hexylphenyl)-dithieno [2,3-d:2’,3’-d’]-s-indaceno [1,2-b:5,6-b’] dithiophene) were prepared by means of spin-coating method, and the influence of the active layer thickness on the device performance was investigated. PBDB-T: ITIC active layers with different thickness were prepared through varying spin coating speed. It was found that the solar cell performance is best when the active layer thickness is 100 nm, corresponding to the spin coating speed of 2000 rpm. Maximum power conversion efficiency of 7.25% with fill factor of 65%, open circuit voltage of 0.85 V and short circuit current density of 13.02 Am/cm2 was obtained.


RSC Advances ◽  
2016 ◽  
Vol 6 (28) ◽  
pp. 23760-23774 ◽  
Author(s):  
Ranjith Krishna Pai ◽  
Ahipa T. N. ◽  
Hemavathi B.

We present a concise review of conjugated polymers based on benzodithiophenes (BDTs) for high-performance polymer solar cells (PSCs).


2014 ◽  
Vol 2 (47) ◽  
pp. 20203-20212 ◽  
Author(s):  
Wei-Hsuan Tseng ◽  
Hsieh-Chih Chen ◽  
Yun-Chen Chien ◽  
Chi-Chang Liu ◽  
Yung-Kang Peng ◽  
...  

A new polymer solar cell with PCE of 6.36% and long-term stability.


2017 ◽  
Vol 8 (30) ◽  
pp. 4393-4402 ◽  
Author(s):  
Nemal S. Gobalasingham ◽  
Seyma Ekiz ◽  
Robert M. Pankow ◽  
Francesco Livi ◽  
Eva Bundgaard ◽  
...  

Direct arylation polymerization (DArP) is used to synthesize a variety of carbazole-based copolymers for evaluation in solar cells.


2013 ◽  
Vol 25 (15) ◽  
pp. 3196-3204 ◽  
Author(s):  
Yang Wang ◽  
Ying Liu ◽  
Shaojie Chen ◽  
Ruixiang Peng ◽  
Ziyi Ge

2018 ◽  
Vol 32 (23) ◽  
pp. 1850269 ◽  
Author(s):  
Mohamed Moustafa ◽  
Tariq Alzoubi

The impact of molybdenum ditelluride (p-type MoTe2) transition metal dichalcogenide (TMDC) material formation as an interfacial layer between CdTe absorber layer and Mo back contact is investigated. The simulation is conducted using the solar cell capacitance simulator (SCAPS) software. Band gap energy, carrier concentration, and layer thickness of the p-MoTe2 have been varied in this study to investigate the possible influences of p-MoTe2 on the electrical properties and the photovoltaic parameters of CdTe thin film solar cells. It has been observed that a thickness of the p-MoTe2 interfacial layer less than 60 nm leads to a decrease in the cell performance. In regard to the effect of the band gap, a maximum efficiency of 16.4% at the optimum energy gap value of 0.95 eV has been obtained at a doping of [Formula: see text]. Additionally, increasing the acceptor carrier concentration [Formula: see text] of MoTe2 enhances the solar cell performance. The solar cell efficiency reaches 15.5% with [Formula: see text] of [Formula: see text] with layer thicknesses above 80 nm. This might be attributed to the possibility of forming a back surface field for the photogenerated electrons, which reduces recombination at the back contact and hence provides a low resistivity contact for holes. The results justify that the MoTe2 interfacial layer mediates an ohmic contact to CdTe films.


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