Namakian Reza, Garzon Maria Alejandra, Tu Qing, Erdemir Ali, Gao Wei
J. Mike Walker'66 Department of Mechanical Engineering, Texas A&M University, College Station, Texas 77843, United States.
Department of Materials Science & Engineering, Texas A&M University, College Station, Texas 77840, United States.
ACS Nano. 2024 Aug 27;18(34):22926-22937. doi: 10.1021/acsnano.4c03903. Epub 2024 Aug 13.
Molecular dynamics simulations are utilized to unravel the temperature-driven phase transition in double-layered butylammonium (BA) methylammonium (MA) lead halide perovskite (BA)(MA)PbI, which holds great promise for a wide range of optoelectronics and sensor applications. The simulations successfully capture the structural transition from low to high symmetry phases with rising temperatures, consistent with experimental observations. The phase transition is initiated at two critical interfaces: the first is between the inorganic and organic layers, where the melting of N-H bonds in BA leads to a significant reduction in hydrogen bonding between BA and iodides, and the second is at the interface between the top and bottom organic layers, where the melting of the tail bonds in BA triggers the phase transition. Following this, BA cations exhibit a patterned and synchronized motion reminiscent of a conical pendulum, displaying a mix of ordered and disordered behaviors prior to evolving into a completely molten and disordered state. While the melting of BA cations is the primary driver of the phase transition, the rotational dynamics of MA cations also plays a critical role in determining the phase transition temperature, influenced by the BA-MA interaction. Such an interaction alters the polarization patterns of MA cations across the phase transition. In particular, an antiparallel polarization pattern is observed in the low-temperature phase. Additionally, displacive elements of the phase transition are identified in the simulations, characterized by the shear and distortion of the inorganic octahedra. Notably, at lower temperatures, the octahedral distortion follows a bimodal distribution, reflecting significant variations in distortion among octahedra. This variation is attributed to an anisotropic hydrogen bonding network between iodides and BA cations. Our study reveals the phenomena and mechanisms extending beyond the order-disorder transition mechanism, suggesting potential phase engineering through strategic tuning of organic and inorganic components.
分子动力学模拟被用于揭示双层丁基铵(BA)甲基铵(MA)铅卤化物钙钛矿(BA)(MA)PbI₃中温度驱动的相变,这在广泛的光电子学和传感器应用中具有巨大潜力。模拟成功捕捉到随着温度升高从低对称相向高对称相的结构转变,与实验观察结果一致。相变在两个关键界面处开始:第一个是无机层和有机层之间,BA中N - H键的熔化导致BA与碘化物之间氢键的显著减少;第二个是顶部和底部有机层之间的界面,BA中尾键的熔化触发相变。在此之后,BA阳离子呈现出类似圆锥摆的有规律且同步的运动,在演变成完全熔融和无序状态之前表现出有序和无序行为的混合。虽然BA阳离子的熔化是相变的主要驱动力,但MA阳离子的旋转动力学在确定相变温度方面也起着关键作用,受BA - MA相互作用的影响。这种相互作用在相变过程中改变了MA阳离子的极化模式。特别是,在低温相中观察到反平行极化模式。此外,在模拟中识别出相变的位移元素,其特征是无机八面体的剪切和畸变。值得注意的是,在较低温度下,八面体畸变呈现双峰分布,反映出八面体之间畸变的显著差异。这种差异归因于碘化物和BA阳离子之间的各向异性氢键网络。我们的研究揭示了超越有序 - 无序转变机制的现象和机制,表明通过对有机和无机组分进行策略性调整来实现潜在的相工程。