Perovskite-quantum dots interface: Deciphering its ultrafast charge carrier dynamics

被引:28
作者
Galar, Pavel [1 ,2 ]
Piatkowski, Piotr [1 ,2 ,4 ]
Thi Tuyen Ngo [3 ]
Gutierrez, Mario [1 ,2 ]
Mora-Sero, Ivan [3 ]
Douhal, Abderrazzak [1 ,2 ]
机构
[1] UCLM, Fac Ciencias Ambientales & Bioquim, Dept Quim Fis, Ave Carlos III S-N, Toledo 45071, Spain
[2] UCLM, INAMOL, Ave Carlos III S-N, Toledo 45071, Spain
[3] Univ Jaume 1, Inst Adv Mat, Av Vicent Sos Baynat S-N, Castellon de La Plana 12006, Spain
[4] Univ Warsaw, Fac Chem, Pasteura 1, PL-02093 Warsaw, Poland
基金
欧洲研究理事会;
关键词
Perovskite; Quantum dots; LEDs; Lighting; Hybrid nanostructures; Electron and hole dynamics; LEAD HALIDE PEROVSKITE; SOLAR-CELLS; RECOMBINATION DYNAMICS; CH3NH3PBI3; PEROVSKITE; RELAXATION DYNAMICS; EXCITED-STATE; DIFFUSION; PBS; TRANSPORT; ELECTRON;
D O I
10.1016/j.nanoen.2018.04.069
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Understanding electron and hole (e,h) transport at semiconductor interfaces is paramount to developing efficient optoelectronic devices. Halide perovskite/semiconductor quantum dots (QDs) have emerged as smart hybrid systems with a huge potential for light emission and energy conversion. However, the dynamics of generated e-h pairs are not fully understood. Ultrafast UV-VIS transient absorption and THz spectroscopies have enabled us to unravel the processes of the e-h recombination within a hybrid film of methylammonium lead triiodide (MAPbI(3)) interacting with different amount of PbS/CdS core/shell QDs. To accurately analyze the complex behavior, we applied a new model for e-h events in this hybrid material. The results obtained with sample having a high concentration of QDs (7.3 mass percentage) indicate: (i) a large population (92%) of the photogenerated charge carriers are affected by QDs presence. The main part of these carriers (85% of the total) in perovskite domain diffuse towards QDs, where they transfer to the interface (electrons) and QD's valence bands (holes) with rate constants of 1.2 x 10(10) s(-1) and 4.6 x 10(10) s(-1), respectively. 7% of these affected charged entities are excitons in the perovskite domain in close vicinity of the interface, and show a recombination rate constant of 3.7 x 10(10) s(-1). (ii) The carriers not affected by QDs presence (8%) recombine through known perovskite deactivation channels. Lowering the QDs mass percentage to 0.24 causes a decrease of electron and hole effective transfer rate constants, and disappearance of excitons. These results provide clues to improve the performance of perovskite/QD based devices.
引用
收藏
页码:471 / 480
页数:10
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