4.8 Article

Thick-Layer Lead Iodide Perovskites with Bifunctional Organic Spacers Allylammonium and Iodopropylammonium Exhibiting Trap-State Emission

期刊

JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
卷 144, 期 14, 页码 6390-6409

出版社

AMER CHEMICAL SOC
DOI: 10.1021/jacs.2c00571

关键词

-

资金

  1. Office of Naval Research [N00014-17-1-2231]
  2. Dr. John N. Nicholson fellowship through Northwestern University
  3. Northwestern Materials Research Science and Engineering Center (NUMRSEC) [DMR-1720139]
  4. Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource [NSF ECCS-2025633]
  5. Texas A&M Engineering Experiment Station (TEES)
  6. Texas A&M Triads for Transformation (T3) grant

向作者/读者索取更多资源

This article introduces three new homologous series of two-dimensional lead iodide perovskites with different organic cations and discusses their structural and technological features. The different organic cations have an impact on the structure and optical properties of the material. The study reveals that the incorporation of specific organic cations leads to lattice distortions and the formation of trap states.
The nature of the organic cation in two-dimensional(2D) hybrid lead iodide perovskites tailors the structural andtechnological features of the resultant material. Herein, we presentthree new homologous series of (100) lead iodide perovskites withthe organic cations allylammonium (AA) containing an unsaturatedC = C group and iodopropylammonium (IdPA) containing iodine onthe organic chain: (AA)(2)MA(n-1)Pb(n)I(3n+1)(n=3-4),[(AA)(x)(IdPA)(1-x)](2)MA(n-1)Pb(n)I(3n+1)(n=1-4), and (Id-PA)(2)MA(n-1)Pb(n)I(3n+1)(n=1-4), as well as their perovskite-relatedsubstructures. We report the in situ transformation of AA organiclayers into IdPA and the incorporation of these cations simulta-neously into the 2D perovskite structure. Single-crystal X-raydiffraction shows that (AA)(2)MA(2)Pb(3)I(10)crystallizes in the spacegroup P2(1)/c with a unique inorganic layer offset (0, <1/2), comprising thefirst example of n= 3 halide perovskite with amonoammonium cation that deviates from the Ruddlesden-Popper (RP) halide structure type. (IdPA)(2)MA(2)Pb(3)I(10) and the alloyed[(AA)(x)(IdPA)(1-x)](2)MA(2)Pb(3)I(10)crystallize in the RP structure, both in space group P2(1)/c. The adjacent I center dot center dot center dot I interlayer distance in(AA)(2)MA(2)Pb(3)I(10) is similar to 5.6 A, drawing the [Pb3I10](4-) layers closer together among all reported n= 3 RP lead iodides. (AA)(2)MA(2)Pb(3)I(10) presents band-edge absorption and photoluminescence (PL) emission at around 2.0 eV that is slightly red-shifted in comparison to(IdPA)(2)MA(2)Pb(3)I(10). The band structure calculations suggest that both (AA)(2)MA(2)Pb(3)I(10) and (IdPA)(2)MA(2)Pb(3)I(10) have in-planeeffective masses around 0.04 m(0) and 0.08 m(0), respectively. IdPA cations have a greater dielectric contribution than AA. The excited-state dynamics investigated by transient absorption (TA) spectroscopy reveal a long-lived (similar to 100 ps) trap state ensemble with broad-band emission; our evidence suggests that these states appear due to lattice distortions induced by the incorporation of IdPA cations.

作者

我是这篇论文的作者
点击您的名字以认领此论文并将其添加到您的个人资料中。

评论

主要评分

4.8
评分不足

次要评分

新颖性
-
重要性
-
科学严谨性
-
评价这篇论文

推荐

暂无数据
暂无数据