Introducing optically polarizable molecules into perovskite solar cells by simultaneously enhanced spin–orbital coupling, suppressed non-radiative recombination and improved transport balance towards enhancing photovoltaic actions

2018 ◽  
Vol 6 (23) ◽  
pp. 6164-6171 ◽  
Author(s):  
Changfeng Han ◽  
Haomiao Yu ◽  
Jiashun Duan ◽  
Kai Lu ◽  
Jia Zhang ◽  
...  

Introducing optically polarizable molecules into perovskite solar cells can enhance photovoltaic actions.

Nano Energy ◽  
2017 ◽  
Vol 38 ◽  
pp. 297-303 ◽  
Author(s):  
Jia Zhang ◽  
Ting Wu ◽  
Jiashun Duan ◽  
Mahshid Ahmadi ◽  
Fangyuan Jiang ◽  
...  

2019 ◽  
Vol 5 (1) ◽  
pp. 44-60 ◽  
Author(s):  
Deying Luo ◽  
Rui Su ◽  
Wei Zhang ◽  
Qihuang Gong ◽  
Rui Zhu

2022 ◽  
Vol 12 (1) ◽  
Author(s):  
Dong In Kim ◽  
Ji Won Lee ◽  
Rak Hyun Jeong ◽  
Jin-Hyo Boo

AbstractOver the past number of years, the power conversion efficiency of perovskite solar cells has remained at 25.5%, reflecting a respectable result for the general incorporation of organometallic trihalide perovskite solar cells. However, perovskite solar cells still suffer from long-term stability issues. Perovskite decomposes upon exposure to moisture, thermal, and UV-A light. Studies related to this context have remained ongoing. Recently, research was mainly conducted on the stability of perovskite against non-radiative recombination. This study improved a critical instability in perovskite solar cells arising from non-radiative recombination and UV-A light using a passivation layer. The passivation layer comprised a polyaniline (PANI) polymer as an interfacial modifier inserted between the active layer and the electron transport layer. Accordingly, the UV-A light did not reach the active layer and confined the Pb2+ ions at PANI passivation layer. This study optimized the perovskite solar cells by controlling the concentration, thickness and drying conditions of the PANI passivation layer. As a result, the efficiency of the perovskite solar cell was achieved 15.1% and showed over 84% maintain in efficiency in the ambient air for one month using the 65 nm PANI passivation layer.


2018 ◽  
Vol 11 (11) ◽  
pp. 3310-3320 ◽  
Author(s):  
Mohammad Mahdi Tavakoli ◽  
Wolfgang Tress ◽  
Jovana V. Milić ◽  
Dominik Kubicki ◽  
Lyndon Emsley ◽  
...  

Non-radiative recombination losses are reduced drastically by addition of adamantylammonium iodide (ADAHI) into the hole transporting layer (HTL) in a perovskite solar cell, resulting in high efficiency (∼22%), increased Voc up to 1245 mV, and enhanced electro-luminescence EQE to 2.5%.


2019 ◽  
Vol 7 (38) ◽  
pp. 21662-21667 ◽  
Author(s):  
Kui Jiang ◽  
Fei Wu ◽  
Guangye Zhang ◽  
Philip C. Y. Chow ◽  
Chao Ma ◽  
...  

An interfacial engineering strategy is successfully developed with a maximum PCE of 20.22%, a high VOC of 1.084 V and a relatively low non-radiative recombination loss in inverted planar perovskite solar cells.


2015 ◽  
Vol 27 (11) ◽  
pp. 1837-1841 ◽  
Author(s):  
Gert-Jan A. H. Wetzelaer ◽  
Max Scheepers ◽  
Araceli Miquel Sempere ◽  
Cristina Momblona ◽  
Jorge Ávila ◽  
...  

Nanophotonics ◽  
2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Waseem Raja ◽  
Michele De Bastiani ◽  
Thomas G. Allen ◽  
Erkan Aydin ◽  
Arsalan Razzaq ◽  
...  

Abstract Metal halide perovskites have emerged in recent years as promising photovoltaic materials due to their excellent optical and electrical properties, enabling perovskite solar cells (PSCs) with certified power conversion efficiencies (PCEs) greater than 25%. Provided radiative recombination is the dominant recombination mechanism, photon recycling – the process of reabsorption (and re-emission) of photons that result from radiative recombination – can be utilized to further enhance the PCE toward the Shockley–Queisser (S-Q) theoretical limit. Geometrical optics can be exploited for the intentional trapping of such re-emitted photons within the device, to enhance the PCE. However, this scheme reaches its fundamental diffraction limits at the submicron scale. Therefore, introducing photonic nanostructures offer attractive solutions to manipulate and trap light at the nanoscale via light coupling into guided modes, as well as localized surface plasmon and surface plasmon polariton modes. This review focuses on light-trapping schemes for efficient photon recycling in PSCs. First, we summarize the working principles of photon recycling, which is followed by a review of essential requirements to make this process efficient. We then survey photon recycling in state-of-the-art PSCs and propose design strategies to invoke light-trapping to effectively exploit photon recycling in PSCs. Finally, we formulate a future outlook and discuss new research directions in the context of photon recycling.


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