Chemical Behavior and Local Structure of the Ruddlesden-Popper and Dion-Jacobson Alloyed Pb/Sn Bromide 2D Perovskites.
Ping FuMichael A QuinteroEugenia S VasileiadouParth RavalClaire WeltonMikael KepenekianGeorge VolonakisJacky EvenYukun LiuChristos D MalliakasYi YangCraig C LaingVinayak P DravidG N Manjunatha ReddyCan LiEdward H SargentMercouri G KanatzidisPublished in: Journal of the American Chemical Society (2023)
The alloyed lead/tin (Pb/Sn) halide perovskites have gained significant attention in the development of tandem solar cells and other optoelectronic devices due to their widely tunable absorption edge. To gain a better understanding of the intriguing properties of Pb/Sn perovskites, such as their anomalous bandgap's dependence on stoichiometry, it is important to deepen the understanding of their chemical behavior and local structure. Herein, we investigate a series of two-dimensional Ruddlesden-Popper (RP) and Dion-Jacobson (DJ) phase alloyed Pb/Sn bromide perovskites using butylammonium (BA) and 3-(aminomethyl)pyridinium (3AMPY) as the spacer cations: (BA) 2 (MA) n -1 Pb x Sn n - x Br 3 n +1 ( n = 1-3) and (3AMPY)(MA) n -1 Pb x Sn n - x Br 3 n +1 ( n = 1-3) through a solution-based approach. Our results show that the ratio and site preference of Pb/Sn atoms are influenced by the layer thickness ( n ) and spacer cations (A'), as determined by single-crystal X-ray diffraction. Solid-state 1 H, 119 Sn, and 207 Pb NMR spectroscopy analysis shows that the Pb atoms prefer the outer layers in n = 3 members: (BA) 2 (MA)Pb x Sn n - x Br 10 and (3AMPY)(MA)Pb x Sn n - x Br 10 . Layered 2D DJ alloyed Pb/Sn bromide perovskites (3AMPY)(MA) n -1 Pb x Sn n - x Br 3 n +1 ( n = 1-3) demonstrate much narrower optical band gaps, lower energy PL emission peaks, and longer carrier lifetimes compared to those of RP analogs. Density functional theory calculations suggest that Pb-rich alloys (Pb:Sn ∼4:1) for n = 1 compounds are thermodynamically favored over 50:50 (Pb:Sn ∼1:1) compositions. From grazing-incidence wide-angle X-ray scattering (GIWAXS), we see that films in the RP phase orient parallel to the substrate, whereas for DJ cases, random orientations are observed relative to the substrate.