FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> and FA(Mn:Pb)I</span><sub><span style="...FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> and FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> perovskite films were prepared and evaluated</span></span><span style="font-family:""><span style="font-family:Verdana;"> through steady and transient absorption spectroscopy. According to the analysis using Elliot’s model, there were no considerable differences except for the absorption intensity between FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> and FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> perovskite films: the value of the optical gap (</span><i><span style="font-family:Verdana;">E</span><sub><span style="font-family:Verdana;">g</span></sub></i><span style="font-family:Verdana;">) and the position of exciton resonance (</span><i><span style="font-family:Verdana;">E</span><sub><span style="font-family:Verdana;">0</span></sub></i><span style="font-family:Verdana;">) were the same. </span><span style="font-family:Verdana;">The femtosecond transient absorption showed biexponential relaxation</span><span style="font-family:Verdana;"> properties of the charge carriers, suggesting that biexcitons are more easily generated in FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> than FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> perovskite. The generation of biexcitons in FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> was also confirmed by the photon pump fluence dependence. Moreover, we were able to estimate the average number of absorbed photons </span><i><span style="font-family:Verdana;"><N></span></i><span style="font-family:Verdana;"> directly from the photon pump power dependence without needing any further experimental measurements such as photoluminescence. Our findings may offer a new way of understanding photoinduced carrier dynamics in perovskite manganites.展开更多
Formamidinium lead triiodide(HC(NH2)2PbI3 or FAPbI3)is a promising light absorber for high-efficiency perovskite solar cells because of its superior light absorption range and thermal stability to CH3NH3PbI3(MAPbI3).U...Formamidinium lead triiodide(HC(NH2)2PbI3 or FAPbI3)is a promising light absorber for high-efficiency perovskite solar cells because of its superior light absorption range and thermal stability to CH3NH3PbI3(MAPbI3).Unfortunately,it is difficult to fabricate high-quality FAPbI3 thin films to surpass the MAPbI3-based cells due to easily forming unwanted but more stable yellow d-phase and thus requiring high annealing-temperature for wanted photovoltaic-active black a-phase.Herein,we reported a novel low-temperature fabrication of highly crystallized a-FAPbI3 film exhibiting uniaxial-oriented nature with large grain sizes up to 2 lm.First-principles energetic calculations predicted that this novel deposition should be ascribed to the formation of a high-energy metastable two-dimensional(2D)intermediate of MAFAPbI3 Cl followed by a spontaneous conversion to a-FAPbI3.The ions exchange reaction during this MAFAPbI3 Cl-FAPbI3 conversion account for the perovskite film uniaxial-oriented grown along the(111)direction.This large-grain and uniaxial-oriented grown a-FAPbI3 based solar cells exhibited an efficiency up to 20.4%accompanying with low density-voltage(J-V)hysteresis and high stability.展开更多
文摘FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> and FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> perovskite films were prepared and evaluated</span></span><span style="font-family:""><span style="font-family:Verdana;"> through steady and transient absorption spectroscopy. According to the analysis using Elliot’s model, there were no considerable differences except for the absorption intensity between FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> and FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> perovskite films: the value of the optical gap (</span><i><span style="font-family:Verdana;">E</span><sub><span style="font-family:Verdana;">g</span></sub></i><span style="font-family:Verdana;">) and the position of exciton resonance (</span><i><span style="font-family:Verdana;">E</span><sub><span style="font-family:Verdana;">0</span></sub></i><span style="font-family:Verdana;">) were the same. </span><span style="font-family:Verdana;">The femtosecond transient absorption showed biexponential relaxation</span><span style="font-family:Verdana;"> properties of the charge carriers, suggesting that biexcitons are more easily generated in FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> than FAPbI</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> perovskite. The generation of biexcitons in FA(Mn:Pb)I</span><sub><span style="font-family:Verdana;">3</span></sub><span style="font-family:Verdana;"> was also confirmed by the photon pump fluence dependence. Moreover, we were able to estimate the average number of absorbed photons </span><i><span style="font-family:Verdana;"><N></span></i><span style="font-family:Verdana;"> directly from the photon pump power dependence without needing any further experimental measurements such as photoluminescence. Our findings may offer a new way of understanding photoinduced carrier dynamics in perovskite manganites.
基金the support of the National Natural Science Foundation of China(21777096,51861145101)the support of the National Natural Science Foundation of China(61722403,11674121)+3 种基金Huoyingdong Grant(151046)the National Key Research and Development Program of China(2016YFB0201204)the support of The Initiative Postdocs Supporting Program(BX20180185)China Postdoctoral Science Foundation(2018M640387)
文摘Formamidinium lead triiodide(HC(NH2)2PbI3 or FAPbI3)is a promising light absorber for high-efficiency perovskite solar cells because of its superior light absorption range and thermal stability to CH3NH3PbI3(MAPbI3).Unfortunately,it is difficult to fabricate high-quality FAPbI3 thin films to surpass the MAPbI3-based cells due to easily forming unwanted but more stable yellow d-phase and thus requiring high annealing-temperature for wanted photovoltaic-active black a-phase.Herein,we reported a novel low-temperature fabrication of highly crystallized a-FAPbI3 film exhibiting uniaxial-oriented nature with large grain sizes up to 2 lm.First-principles energetic calculations predicted that this novel deposition should be ascribed to the formation of a high-energy metastable two-dimensional(2D)intermediate of MAFAPbI3 Cl followed by a spontaneous conversion to a-FAPbI3.The ions exchange reaction during this MAFAPbI3 Cl-FAPbI3 conversion account for the perovskite film uniaxial-oriented grown along the(111)direction.This large-grain and uniaxial-oriented grown a-FAPbI3 based solar cells exhibited an efficiency up to 20.4%accompanying with low density-voltage(J-V)hysteresis and high stability.