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Article: In Situ Tin(II) Complex Antisolvent Process Featuring Simultaneous Quasi‐Core–Shell Structure and Heterojunction for Improving Efficiency and Stability of Low‐Bandgap Perovskite Solar Cells
Title | In Situ Tin(II) Complex Antisolvent Process Featuring Simultaneous Quasi‐Core–Shell Structure and Heterojunction for Improving Efficiency and Stability of Low‐Bandgap Perovskite Solar Cells |
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Authors | |
Keywords | grain boundary passivation mixed Pb‐Sn perovskite solar cells perovskite heterostructures quasi‐core–shell structures |
Issue Date | 2020 |
Publisher | Wiley - VCH Verlag GmbH & Co. KGaA. The Journal's web site is located at http://onlinelibrary.wiley.com/journal/10.1002/(ISSN)1614-6840 |
Citation | Advanced Energy Materials, 2020, v. 10 n. 8, p. article no. 1903013 How to Cite? |
Abstract | Unlike Pb‐based perovskites, it is still a challenge for realizing the targets of high performance and stability in mixed Pb–Sn perovskite solar cells owing to grain boundary traps and chemical changes in the perovskites. In this work, proposed is the approach of in‐situ tin(II) inorganic complex antisolvent process for specifically tuning the perovskite nucleation and crystal growth process. Interestingly, uniquely formed is the quasi‐core–shell structure of Pb–Sn perovskite–tin(II) complex as well as heterojunction perovskite structure at the same time for achieving the targets. The core–shell structure of Pb–Sn perovskite crystals covered by a tin(II) complex at the grain boundaries effectively passivates the trap states and suppresses the nonradiative recombination, leading to longer carrier lifetime. Equally important, the perovskite heterostructure is intentionally formed at the perovskite top region for enhancing the carrier extraction. As a result, the mixed Pb–Sn low‐bandgap perovskite device achieves a high power conversion efficiency up to 19.03% with fill factor over 0.8, which is among the highest fill factor in high‐performance Pb–Sn perovskite solar cells. Remarkably, the device fail time under continuous light illumination is extended by over 18.5‐folds from 30 to 560 h, benefitting from the protection of the quasi‐core–shell structure. |
Persistent Identifier | http://hdl.handle.net/10722/287660 |
ISSN | 2023 Impact Factor: 24.4 2023 SCImago Journal Rankings: 8.748 |
ISI Accession Number ID |
DC Field | Value | Language |
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dc.contributor.author | LI, C | - |
dc.contributor.author | MA, R | - |
dc.contributor.author | HE, X | - |
dc.contributor.author | Yang, T | - |
dc.contributor.author | Zhou, Z | - |
dc.contributor.author | Yang, S | - |
dc.contributor.author | Liang, Y | - |
dc.contributor.author | Sun, XW | - |
dc.contributor.author | Wang, J | - |
dc.contributor.author | Yan, Y | - |
dc.contributor.author | Choy, WCH | - |
dc.date.accessioned | 2020-10-05T12:01:22Z | - |
dc.date.available | 2020-10-05T12:01:22Z | - |
dc.date.issued | 2020 | - |
dc.identifier.citation | Advanced Energy Materials, 2020, v. 10 n. 8, p. article no. 1903013 | - |
dc.identifier.issn | 1614-6832 | - |
dc.identifier.uri | http://hdl.handle.net/10722/287660 | - |
dc.description.abstract | Unlike Pb‐based perovskites, it is still a challenge for realizing the targets of high performance and stability in mixed Pb–Sn perovskite solar cells owing to grain boundary traps and chemical changes in the perovskites. In this work, proposed is the approach of in‐situ tin(II) inorganic complex antisolvent process for specifically tuning the perovskite nucleation and crystal growth process. Interestingly, uniquely formed is the quasi‐core–shell structure of Pb–Sn perovskite–tin(II) complex as well as heterojunction perovskite structure at the same time for achieving the targets. The core–shell structure of Pb–Sn perovskite crystals covered by a tin(II) complex at the grain boundaries effectively passivates the trap states and suppresses the nonradiative recombination, leading to longer carrier lifetime. Equally important, the perovskite heterostructure is intentionally formed at the perovskite top region for enhancing the carrier extraction. As a result, the mixed Pb–Sn low‐bandgap perovskite device achieves a high power conversion efficiency up to 19.03% with fill factor over 0.8, which is among the highest fill factor in high‐performance Pb–Sn perovskite solar cells. Remarkably, the device fail time under continuous light illumination is extended by over 18.5‐folds from 30 to 560 h, benefitting from the protection of the quasi‐core–shell structure. | - |
dc.language | eng | - |
dc.publisher | Wiley - VCH Verlag GmbH & Co. KGaA. The Journal's web site is located at http://onlinelibrary.wiley.com/journal/10.1002/(ISSN)1614-6840 | - |
dc.relation.ispartof | Advanced Energy Materials | - |
dc.rights | This is the peer reviewed version of the following article: [FULL CITE], which has been published in final form at [Link to final article using the DOI]. This article may be used for non-commercial purposes in accordance with Wiley Terms and Conditions for Use of Self-Archived Versions. | - |
dc.subject | grain boundary passivation | - |
dc.subject | mixed Pb‐Sn perovskite solar cells | - |
dc.subject | perovskite heterostructures | - |
dc.subject | quasi‐core–shell structures | - |
dc.title | In Situ Tin(II) Complex Antisolvent Process Featuring Simultaneous Quasi‐Core–Shell Structure and Heterojunction for Improving Efficiency and Stability of Low‐Bandgap Perovskite Solar Cells | - |
dc.type | Article | - |
dc.identifier.email | Choy, WCH: chchoy@eee.hku.hk | - |
dc.identifier.authority | Choy, WCH=rp00218 | - |
dc.description.nature | link_to_subscribed_fulltext | - |
dc.identifier.doi | 10.1002/aenm.201903013 | - |
dc.identifier.scopus | eid_2-s2.0-85078615224 | - |
dc.identifier.hkuros | 315685 | - |
dc.identifier.volume | 10 | - |
dc.identifier.issue | 8 | - |
dc.identifier.spage | article no. 1903013 | - |
dc.identifier.epage | article no. 1903013 | - |
dc.identifier.isi | WOS:000507569900001 | - |
dc.publisher.place | Germany | - |
dc.identifier.issnl | 1614-6832 | - |