18 Aug 11:45
Energy Environ. Sci., 2020, 13,2024-2046
DOI: 10.1039/D0EE00788A, Perspective
Alexander J. Knight, Laura M. Herz
Halide segregation represents a severe stability problem for certain mixed-halide perovskites. Here we explore a myriad of methods for mitigating halide segregation, including several largely unexplored approaches that show significant promise.
The content of this RSS Feed (c) The Royal Society of Chemistry
02 Jul 13:32
by Hongyao Xie†, Shiqiang Hao‡, Jinke Bao§, Tyler J. Slade†, G. Jeffrey Snyder‡, Christopher Wolverton‡, and Mercouri G. Kanatzidis*†

Journal of the American Chemical Society
DOI: 10.1021/jacs.0c03427
28 Jun 13:52
by Peng Huang†?, Manju§?, Samrana Kazim†‡, Gangala Sivakumar§, Manuel Salado†, Rajneesh Misra*§, and Shahzada Ahmad*†‡

ACS Applied Materials & Interfaces
DOI: 10.1021/acsami.0c03584
28 Jun 12:51
Energy Environ. Sci., 2020, 13,1154-1186
DOI: 10.1039/C9EE03757H, Review Article
Fei Zhang, Haipeng Lu, Jinhui Tong, Joseph J. Berry, Matthew C. Beard, Kai Zhu
Recent achievements of 2D perovskites for various optoelectronic applications along with their basic properties and future opportunities are discussed.
The content of this RSS Feed (c) The Royal Society of Chemistry
24 Jun 08:31
by Yepin Zhao,
Pengchen Zhu,
Minhuan Wang,
Shu Huang,
Zipeng Zhao,
Shaun Tan,
Tae‐Hee Han,
Jin‐Wook Lee,
Tianyi Huang,
Rui Wang,
Jingjing Xue,
Dong Meng,
Yu Huang,
Jaime Marian,
Jia Zhu,
Yang Yang
A polymerization‐assisted grain growth strategy in the sequential deposition method of perovskite thin films is demonstrated by triggering a polymerization process during PbI2 film annealing. This strategy effectively passivates undercoordinated lead ions, reduces defect density, and boosts power conversion efficiency up to 23.0%, together with a prolonged lifetime.
Abstract
Intrinsically, detrimental defects accumulating at the surface and grain boundaries limit both the performance and stability of perovskite solar cells. Small molecules and bulkier polymers with functional groups are utilized to passivate these ionic defects but usually suffer from volatility and precipitation issues, respectively. Here, starting from the addition of small monomers in the PbI2 precursor, a polymerization‐assisted grain growth strategy is introduced in the sequential deposition method. With a polymerization process triggered during the PbI2 film annealing, the bulkier polymers formed will be adhered to the grain boundaries, retaining the previously established interactions with PbI2. After perovskite formation, the polymers anchored on the boundaries can effectively passivate undercoordinated lead ions and reduce the defect density. As a result, a champion power conversion efficiency (PCE) of 23.0% is obtained, together with a prolonged lifetime where 85.7% and 91.8% of the initial PCE remain after 504 h continuous illumination and 2208 h shelf storage, respectively.
24 Jun 08:25
by Hobeom Kim,
Mingyuan Pei,
Yonghui Lee,
Albertus A. Sutanto,
Sanghyun Paek,
Valentin I. E. Queloz,
Aron J. Huckaba,
Kyung Taek Cho,
Hyung Joong Yun,
Hoichang Yang,
Mohammad Khaja Nazeeruddin
Self‐crystallized multifunctional 2D perovskite (M2P) is formed on top of a 3D perovskite light absorber. The M2P layer performs as a hole‐transfer facilitator and a surface‐trap passivator in perovskite solar cells (PSCs). PSCs using the developed 3D/2D perovskites achieve a power conversion efficiency of 20.79% with highly improved long‐term stability compared to devices without M2P.
Abstract
Recently, perovskite solar cells (PSC) with high power‐conversion efficiency (PCE) and long‐term stability have been achieved by employing 2D perovskite layers on 3D perovskite light absorbers. However, in‐depth studies on the material and the interface between the two perovskite layers are still required to understand the role of the 2D perovskite in PSCs. Self‐crystallization of 2D perovskite is successfully induced by deposition of benzyl ammonium iodide (BnAI) on top of a 3D perovskite light absorber. The self‐crystallized 2D perovskite can perform a multifunctional role in facilitating hole transfer, owing to its random crystalline orientation and passivating traps in the 3D perovskite. The use of the multifunctional 2D perovskite (M2P) leads to improvement in PCE and long‐term stability of PSCs both with and without organic hole transporting material (HTM), 2,2′,7,7′‐tetrakis‐(N,N‐di‐p‐methoxyphenyl‐amine)‐9,9′‐spirobifluorene (spiro‐OMeTAD) compared to the devices without the M2P.
24 Jun 08:21
by Guohua Wu,
Hua Li,
Jian Cui,
Yaohong Zhang,
Selina Olthof,
Shuai Chen,
Zhike Liu,
Dapeng Wang,
Shengzhong (Frank) Liu
A strategy is demonstrated for efficacious regulation of perovskite crystallinity using glycolic acid (GA) against nonvolatile thioglycolic acid (TGA) following dimethyl sulfoxide sublimation, resulting in enhanced device performance. A champion power conversion efficiency as high as 21.32% is achieved for the GA‐based device, which is almost 13% or 20% higher than those of the control device or TGA‐based device.
Abstract
A strategy for efficaciously regulating perovskite crystallinity is proposed by using a volatile solid glycolic acid (HOCH2COOH, GA) in an FA0.85MA0.15PbI3 (FA: HC(NH2)2; MA: CH3NH3) perovskite precursor solution that is different from the common additive approach. Accompanied with the first dimethyl sulfoxide sublimation process, the subsequent sublimation of GA before 150 °C in the FA0.85MA0.15PbI3 perovskite film can artfully regulate the perovskite crystallinity without any residual after annealing. The improved film formation upon GA modification induced by the strong interaction between GA and Pb2+ delivers a champion power conversion efficiency (PCE) as high as 21.32%. In order to investigate the role of volatility in perovskite solar cells (PSCs), nonvolatile thioglycolic acid (HSCH2COOH, TGA) with a similar structure to GA is utilized as an additive reference. Large perovskite grains are obtained by TGA modification but with obvious pinholes, which directly leads to an increased defect density accompanied by a decline in PCE. Encouragingly, the champion PCE achieved for GA‐based PSC device (21.32%) is almost 13% or 20% higher than those of the control device or TGA‐based device. In addition, GA‐modified PSCs exhibit the best stability in light‐, thermal‐, and humidity‐based tests due to the improved film formation.
24 Jun 08:18
by Liangyou Lin,
Timothy W. Jones,
Jacob Tse‐Wei Wang,
Andre Cook,
Ngoc Duy Pham,
Noel W. Duffy,
Blago Mihaylov,
Mihaela Grigore,
Kenrick F. Anderson,
Benjamin C. Duck,
Hongxia Wang,
Jian Pu,
Jian Li,
Bo Chi,
Gregory J. Wilson
In article https://doi.org/10.1002/smll.2019014661901466, Bo Chi, Gregory J. Wilson, and co‐workers investigate superior electronic properties of nanostructured tin (IV) oxide (SnO2) as an ideal inorganic electron transport layer (ETL) in n–i–p perovskite solar cells. The bilayer ETL architecture attaining impressive power conversion efficiency (PCE) greater than 20% is depicted.
24 Jun 08:08
by Tingwei He,
Yuanzhi Jiang,
Xiangyu Xing,
Mingjian Yuan
Perovskites with different dimensional structures attract wide attention in the field of photovoltaics. There are three main perovskite structures that can be obtained by tuning the A‐site cations, i.e., 3D perovskite, reduced‐dimensional perovskite, and 2D/3D hybrid perovskite, which exhibit different properties, characters, and intrinsic weaknesses. With the use of efficient and targeted tactics, such materials show great potential for perovskite solar cells.
Abstract
Organic–inorganic hybrid lead‐halide perovskite materials (ABX3) have attracted widespread attention in the field of photovoltaics owing to their impressive optical and electrical properties. However, obstacles still exist in the commercialization of perovskite photovoltaics, such as poor stability, hysteresis, and human toxicity. A‐site cation engineering is considered to be a powerful tool to tune perovskite structures and the resulting optoelectronic properties. Based on the selection and combination of A‐site cations, three types of perovskite structures, i.e., 3D perovskite, reduced‐dimensional (2D/quasi‐2D) perovskite, and 2D/3D hybrid perovskite can be formed. Herein, the remarkable breakthroughs resulting from these three perovskite structures are summarized, and their corresponding properties and characteristics, as well as their intrinsic disadvantages, are highlighted. By summarizing recent research progress, a new viewpoint for improving the performance and stability of perovskite photovoltaics is provided.
22 May 06:06
by Jianxing Xia,
Junsheng Luo,
Hua Yang,
Fengjiao Zhao,
Zhongquan Wan,
Haseeb Ashraf Malik,
Yu Shi,
Keli Han,
Xiaojun Yao,
Chunyang Jia
The undercoordinated ionic defects at heterojunction interfaces remain challenges that limit the performances and stability of perovskite photoelectric devices. A self‐phase separated doping strategy is developed to link multilayer heterojunction interfaces including both the energy level and trap states, paving a novel route for nonequilibrium distributed dopants to solve the key challenge of interface defects.
Abstract
In perovskite solar cells (PSCs), the interfaces of the halide perovskite/electron transport layer (ETL) and ETL/metal oxide electrode (MOE) always attract and trap free carriers via the surface electrostatic force, altering quasi‐Fermi level (E
Fq) splitting of contact interfaces, and significantly limit the charge extraction efficiency and intrinsic stability of devices. Herein, a graded “bridge” is first reported to link the MOE and perovskite interfaces by self vertical phase separation doping (PSD), diminishing the side effect of notorious ionic defects via both reinforced interface E
bi and the vacancies filling. Experimental and theoretical results prove that the inhomogeneous distribution of CsF in the bulk or surface of PC61BM would not only form metal–oxygen (M–O) dipole on MOE, reinforcing the interface E
bi, but also create a graded energy bridge to alleviate the disadvantage of band offset raised by the enhanced interface E
bi, which significantly avoid the carrier accumulation and recombination at defective interfaces. Employing PSD, the power conversion efficiency of the devices approaches 21% with a high open‐circuit voltage (1.148 V) and delivers a high stability of 89% after aging 60 days in atmosphere without encapsulation, which is the highest efficiency of organic electron transport layers for n–i–p PSCs.
22 May 06:03
by Ying Zhang,
Delong Liu,
Tsz‐Ki Lau,
Lingling Zhan,
Dong Shen,
Patrick W. K. Fong,
Cenqi Yan,
Shaoqing Zhang,
Xinhui Lu,
Chun‐Sing Lee,
Jianhui Hou,
Hongzheng Chen,
Gang Li
Incorporation a small portion of a novel polymer donor named PBT(E)BTz with a deeper highest occupied molecular orbital level than the host materials is proven promising to construct highly efficient ternary polymer solar cells (PSCs). In addition to the role of a “solid additive” for ternary PSCs, PBT(E)BTz shows great potential to be a thermal and light stabilizer in ternary PSCs.
Abstract
Ternary strategies have attracted extensive attention due to their potential in improving power conversion efficiencies (PCEs) of single‐junction polymer solar cells (PSCs). In this work, a novel wide bandgap polymer donor (E
g
opt ≈ 2.0 eV) named PBT(E)BTz with a deep highest occupied molecular orbital (HOMO) level (≈−5.73 eV) is designed and synthesized. PBT(E)BTz is first incorporated as the third component into the classic PBDB‐T‐SF:IT‐4F binary PSC system to fabricate efficient ternary PSCs. A higher PCE of 13.19% is achieved in the ternary PSCs with a 5% addition of PBT(E)BTz over binary PSCs (12.14%). Similarly, addition of PBT(E)BTz improves the PCE for PBDB‐T:IT‐M binary PSCs from 10.50% to 11.06%. The study shows that the improved PCE in ternary PSCs is mainly attributed to the suppressed charge carrier recombination and more balanced charge transport. The generality of PBT(E)BTz as a third component is further evidenced in another efficient binary PSC system—PBDB‐TF:BTP‐4Cl: an optimized PCE of 16.26% is realized in the ternary devices. This work shows that PBT(E)BTz possessing a deep HOMO level as an additional component is an effective ternary PSC construction strategy toward enhancing device performance. Furthermore, the ternary device with 5% PBT(E)BTz displays better thermal and light stability over binary devices.
22 May 03:42
by Jianxing Xia,
Junsheng Luo,
Hua Yang,
Fengjiao Zhao,
Zhongquan Wan,
Haseeb Ashraf Malik,
Yu Shi,
Keli Han,
Xiaojun Yao,
Chunyang Jia
The undercoordinated ionic defects at heterojunction interfaces remain challenges that limit the performances and stability of perovskite photoelectric devices. A self‐phase separated doping strategy is developed to link multilayer heterojunction interfaces including both the energy level and trap states, paving a novel route of nonequilibrium distributed dopant to solve the key challenge of interface defects.
Abstract
In perovskite solar cells (PSCs), the interfaces of the halide perovskite/electron transport layer (ETL) and ETL/metal oxide electrode (MOE) always attract and trap free carriers via the surface electrostatic force, altering quasi‐Fermi level (E
Fq) splitting of contact interfaces, and significantly limit the charge extraction efficiency and intrinsic stability of devices. Herein, a graded “bridge” is first reported to link the MOE and perovskite interfaces by self vertical phase separation doping (PSD), diminishing the side effect of notorious ionic defects via both reinforced interface E
bi and the vacancies filling. Experimental and theoretical results prove that the inhomogeneous distribution of CsF in the bulk or surface of PC61BM would not only form metal–oxygen (M–O) dipole on MOE, reinforcing the interface E
bi, but also create a graded energy bridge to alleviate the disadvantage of band offset raised by the enhanced interface E
bi, which significantly avoid the carrier accumulation and recombination at defective interfaces. Employing PSD, the power conversion efficiency of the devices approaches 21% with a high open‐circuit voltage (1.148 V) and delivers a high stability of 89% after aging 60 days in atmosphere without encapsulation, which is the highest efficiency of organic electron transport layers for n–i–p PSCs.
22 May 03:30
by Jianan Wang,
Huilei Shi,
Niansheng Xu,
Jing Zhang,
Yi Yuan,
Ming Lei,
Lidong Wang,
Peng Wang
The aza[5]helicene‐based hole‐transporter is superior to its congener with the planar N‐annulated perylene π‐linker. This study has highlighted that the use of a helical π‐linker for donor−π linker−donor typed organic semiconductors can retain stronger intermolecular π⋅⋅⋅π interactions and attenuated interface charge recombination, leading to better power conversion efficiency of perovskite solar cells.
Abstract
The superior role of helical π‐linkers is demonstrated for the design of donor−π linker−donor typed molecular semiconductors in perovskite solar cells (PSCs). Flat N‐annulated perylene (NP) and contorted aza[5]helicene (A5H) are side‐functionalized with methoxyphenyl and end‐capped with dimethoxydiphenylamine electron‐donor to afford two small‐molecule hole‐transporters J3 and J4. For methoxyphenyl functionalized π‐linkers, intermolecular π⋅⋅⋅π interactions in planar NP exist more extensively than those in helical A5H. However, for the dimethoxydiphenylamine derived hole‐transporters with high highest occupied molecular orbital energy levels, a part of the π⋅⋅⋅π interaction remains for J4 with A5H, while this desirable effect for charge transport is completely deprived for J3 with NP. Thus, the theoretically predicted hole mobility of J4 single‐crystal is even over two times higher than that of J3 one. Because of the larger size of the molecular aggregate, the hole mobility of the spin‐coated J4 thin film is also over three times as high as that of the J3 analog. Due to the reduced transport resistance and enhanced recombination resistance, PSCs with J4 exhibit a power conversion efficiency of 21.0% at standard air mass 1.5 global conditions, which is higher than that of 19.4% with J3 and that of 20.3% with spiro‐OMeTAD control.
22 May 03:18
by Lei Zhu,
Ming Zhang,
Guanqing Zhou,
Tianyu Hao,
Jinqiu Xu,
Jing Wang,
Chaoqun Qiu,
Nathaniel Prine,
Jazib Ali,
Wei Feng,
Xiaodan Gu,
Zaifei Ma,
Zheng Tang,
Haiming Zhu,
Lei Ying,
Yongming Zhang,
Feng Liu
In article number https://doi.org/10.1002/aenm.2019042341904234, Feng Liu and co‐workers report a detailed structure‐performance relationship to help understand the success of Y6 non‐fullerene acceptors. Through the analysis of the single crystal structure of Y6, it is found that Y6 forms a polymer‐like conjugated backbone through its banana‐shaped structure and π‐π interactions between molecules, and forms a 2D electron transport network under the ordered arrangement of the lattice.
22 May 03:14
by Miao Zeng,
Xiaojing Wang,
Ruijie Ma,
Weiya Zhu,
Yuan Li,
Zhongxin Chen,
Jiawen Zhou,
Wenqiang Li,
Tao Liu,
Zhicai He,
He Yan,
Fei Huang,
Yong Cao
The doping of poly(3,4‐ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) with dopamine is reported. The doping of dopamine endows PEDOT:PSS with enhanced work function and conductivity. This work provides an efficient strategy to enhance the performances of organic solar cells.
Abstract
Poly(3,4‐ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) has been is applied as hole transport material in organic electronic devices for more than 20 years. However, the redundant sulfonic acid group of PEDOT:PSS has often been overlooked. Herein, PEDOT:PSS‐DA is prepared via a facile doping of PEDOT:PSS with dopamine hydrochloride (DA·HCl) which reacts with the redundant sulfonic acid of PSS. The PEDOT:PSS‐DA film exhibits enhanced work function and conductivity compared to those of PEDOT:PSS. PEDOT:PSS‐DA‐based devices show a power conversion efficiency of 16.55% which is the highest in organic solar cells (OSCs) with (poly[(2,6‐(4,8‐bis(5‐(2‐ethylhexyl)‐4‐fluorothiophen‐2‐yl)benzo[1,2‐b:4,5‐b′]dithio‐phene))‐co‐(1,3‐di(5‐thiophene‐2‐yl)‐5,7‐bis(2‐ethylhexyl)‐benzo[1,2‐c:4,5‐c′]dithiophene‐4,8‐dione))] (PM6):(2,2′‐((2Z,2′Z)‐((12,13‐bis(2‐ethylhexyl)‐3,9‐diundecyl‐12,13‐dihydro‐[1,2,5]thiadiazolo[3,4‐e]thieno[2′′,3′:4′,5′]thieno[2′,3′:4,5]pyrrolo[3,2‐g]thieno[2′,3′:4,5]thieno[3,2‐b]indole‐2,10‐diyl)bis(methanylylidene))bis(5,6‐difluoro‐3‐oxo‐2,3‐dihydro‐1H‐indene‐2,1‐diylidene))dimalononitrile) (Y6) as the active layer. Furthermore, PEDOT:PSS‐DA also exhibits enhanced performance in three other donor/acceptor systems, exhibiting high compatibility in OSCs. This work demonstrates that doping PEDOT:PSS with various amino derivatives is a potentially efficient strategy to enhance the performance of PEDOT:PSS in organic electronic devices.
18 May 08:57
by Pei Cheng* and Yang Yang*

Accounts of Chemical Research
DOI: 10.1021/acs.accounts.0c00157
18 May 08:45
by Nicola Gasparini*†?, Sri Harish Kumar Paleti†?, Jules Bertrandie†, Guilong Cai‡, Guichuan Zhang§, Andrew Wadsworth?, Xinhui Lu‡, Hin-Lap Yip§, Iain McCulloch†?, and Derya Baran*†

ACS Energy Letters
DOI: 10.1021/acsenergylett.0c00604
18 May 08:44
by Randi Azmi†, Naufan Nurrosyid†‡, Sang-Hak Lee†, Muhibullah Al Mubarok†, Wooseop Lee?, Sunbin Hwang§, Wenping Yin?, Tae Kyu Ahn?, Tae-Wook Kim§, Du Yeol Ryu?, Young Rag Do*‡, and Sung-Yeon Jang*†

ACS Energy Letters
DOI: 10.1021/acsenergylett.0c00596
18 May 08:44
by Faming Li?†‡, Yiran Xie?†‡, Yuchao Hu†‡, Mingzhu Long§, Yifeng Zhang†‡, Jianbin Xu§, Minchao Qin?, Xinhui Lu?, and Mingzhen Liu*†‡

ACS Energy Letters
DOI: 10.1021/acsenergylett.0c00286
18 May 08:41
by Shuixing Li, Chang-Zhi Li, Minmin Shi, and Hongzheng Chen*

ACS Energy Letters
DOI: 10.1021/acsenergylett.0c00537
18 May 08:38
by Fang-Xiao Chen†, Ran Qin†, Ruoxi Xia‡, Yingzhu Zhang†, Lijian Zuo§, Hin-Lap Yip‡, Hongzheng Chen†, and Chang-Zhi Li*†

ACS Energy Letters
DOI: 10.1021/acsenergylett.0c00857
16 Jan 07:58
by Nikita Drigo†, Cristina Roldan-Carmona†, Marius Franckevic?ius‡, Kun-Han Lin§, Rokas Gegevic?ius‡, Hobeom Kim†, Pascal A. Schouwink?, Albertus A. Sutanto†, Selina Olthof?, Muhammad Sohail?, Klaus Meerholz?, Vidmantas Gulbinas‡, Cle´mence Corminboeuf§, Sanghyun Paek*†, and Mohammad Khaja Nazeeruddin*†

Journal of the American Chemical Society
DOI: 10.1021/jacs.9b07166
16 Jan 07:57
by Chenkai Sun†‡?, Shucheng Qin†‡?, Rui Wang§, Shanshan Chen??, Fei Pan†‡, Beibei Qiu†‡, Ziya Shang†‡, Lei Meng†, Chunfeng Zhang§, Min Xiao§, Changduk Yang?, and Yongfang Li*†‡#

Journal of the American Chemical Society
DOI: 10.1021/jacs.9b09939
12 Jan 05:50
by Shuai Zhao*†, Chunfeng Lan‡, Huanhuan Li†, Chu Zhang§, and Tingli Ma*§?

The Journal of Physical Chemistry C
DOI: 10.1021/acs.jpcc.9b08450
12 Jan 05:46
by Sergey Tsarev*†, Tatiana S. Dubinina‡§, Sergey Yu. Luchkin†, Ivan S. Zhidkov?, Ernst Z. Kurmaev??, Keith J. Stevenson†, and Pavel A. Troshin†§

The Journal of Physical Chemistry C
DOI: 10.1021/acs.jpcc.9b10709
12 Jan 05:37
by Ya-Qing Liu†‡, Dongshan Wei§, Hong-Liang Cui*†‡, and De-Qiang Wang*‡

ACS Applied Materials & Interfaces
DOI: 10.1021/acsami.9b18452
12 Jan 05:35
by Shurong Wang†‡, Hui Cao*†, Xuhao Liu‡, Yangyang Liu‡, Tao Tao*†, Jinwei Sun†, and Mingdao Zhang*‡

ACS Applied Materials & Interfaces
DOI: 10.1021/acsami.9b20054
12 Jan 05:31
by Wen Wang, Fei Qin, Xiaoyu Zhu, Yang Liu, Xueshi Jiang, Lulu Sun, Cong Xie, and Yinhua Zhou*

ACS Applied Materials & Interfaces
DOI: 10.1021/acsami.9b17321
12 Jan 05:28
by Lina Li†, Xitao Liu†, Chao He†, Sasa Wang†‡, Chengmin Ji†, Xinyuan Zhang†‡, Zhihua Sun†, Sangen Zhao†, Maochun Hong†, and Junhua Luo*†

Journal of the American Chemical Society
DOI: 10.1021/jacs.9b11341
12 Jan 05:28
by Jesu´s Jime´nez-Lo´pez†‡, Bianka M. D. Puscher§, Dirk M. Guldi*§, and Emilio Palomares*†?

Journal of the American Chemical Society
DOI: 10.1021/jacs.9b09182
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