Passivation of Triple Cation perovskites using Guanidinium Iodide in inverted solar cells for improved open-circuit voltage and stability

Author(s):  
Aditya S Yerramilli ◽  
Yuanqing Chen ◽  
Terry L. Alford

Inverted device architectures in perovskite research were promising for faster commercialization given the simple processing routes and choice of hole transport materials such as PEDOT. However, the crystallization of perovskite...

NANO ◽  
2019 ◽  
Vol 14 (10) ◽  
pp. 1950127 ◽  
Author(s):  
Farhad Jahantigh ◽  
S. M. Bagher Ghorashi

Perovskite solar cells have recently been considered to be an auspicious candidate for the advancement of future photovoltaic research. A power conversion efficiency (PCE) as high as 22% has been reported to be reached, which can be obtained through an inexpensive and high-throughput solution process. Modeling and simulation of these cells can provide deep insights into their fundamental mechanism of performance. In this paper, two different perovskite solar cells are designed by using COMSOL Multiphysics to optimize the thickness of each layer and the overall thickness of the cell. Electric potential, electron and hole concentrations, generation rate, open-circuit voltage, short-circuit current and the output power were calculated. Finally, PCEs of 20.7% and 26.1% were predicted. Afterwards, according to the simulation results, the role of the hole transport layer (HTL) was investigated and the optimum thickness of the perovskite was measured to be 200[Formula: see text]nm for both cells. Therefore, the spin coating settings are selected so that a coating with this thickness for cell 1 is deposited. In order to compare the performance of HTM layer, solar cells with a Spiro-OMeTAD HTM and without the HTM layer in their structure were fabricated. According to the obtained photovoltaic properties, the solar cell made with Spiro-OMeTAD has a more favorable open-circuit voltage ([Formula: see text]), short-circuit current density ([Formula: see text]), fill factor (FF) and PCE compared to the cell without the HTM layer. Also, hysteresis depends strongly on the perovskite grain size, because large average grain size will lead to an increase in the grain’s contact surface area and a decrease in the density of grain boundaries. Finally, according to the results, it was concluded that, in the presence of a hole transport layer, ion transfer was better and ion accumulation was less intense, and therefore, the hysteresis decreases.


2019 ◽  
Vol 7 (32) ◽  
pp. 18971-18979 ◽  
Author(s):  
Tian Du ◽  
Weidong Xu ◽  
Matyas Daboczi ◽  
Jinhyun Kim ◽  
Shengda Xu ◽  
...  

Reduction in p-doping of the organic hole transport layer (HTL) leads to substantial improvements in PV performance in planar p–i–n perovskite solar cells.


2017 ◽  
Vol 10 (5) ◽  
pp. 1207-1212 ◽  
Author(s):  
Juan-Pablo Correa-Baena ◽  
Wolfgang Tress ◽  
Konrad Domanski ◽  
Elham Halvani Anaraki ◽  
Silver-Hamill Turren-Cruz ◽  
...  

Dopants in the hole transport layer limit the open-circuit voltage of perovskite solar cells.


Nanoscale ◽  
2019 ◽  
Vol 11 (18) ◽  
pp. 8776-8784 ◽  
Author(s):  
Zhiqi Li ◽  
Jiajun Dong ◽  
Wenbin Han ◽  
Guanhua Ren ◽  
Chunyu Liu ◽  
...  

To overcome the intrinsic chemical-reduction-activity of highly p-doped PEDOT:PSS and improve the open-circuit voltage of planar inverted perovskite solar cells, an oxidized carbon nanorod is developed and incorporated into a PEDOT:PSS hole transport layer.


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