Loading…

Small‐Band‐Gap Halide Double Perovskites

Despite their compositional versatility, most halide double perovskites feature large band gaps. Herein, we describe a strategy for achieving small band gaps in this family of materials. The new double perovskites Cs2AgTlX6 (X=Cl (1) and Br (2)) have direct band gaps of 2.0 and 0.95 eV, respectively...

Full description

Saved in:
Bibliographic Details
Published in:Angewandte Chemie 2018-09, Vol.130 (39), p.12947-12952
Main Authors: Slavney, Adam H., Leppert, Linn, Saldivar Valdes, Abraham, Bartesaghi, Davide, Savenije, Tom J., Neaton, Jeffrey B., Karunadasa, Hemamala I.
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:Despite their compositional versatility, most halide double perovskites feature large band gaps. Herein, we describe a strategy for achieving small band gaps in this family of materials. The new double perovskites Cs2AgTlX6 (X=Cl (1) and Br (2)) have direct band gaps of 2.0 and 0.95 eV, respectively, which are approximately 1 eV lower than those of analogous perovskites. To our knowledge, compound 2 displays the lowest band gap for any known halide perovskite. Unlike in AIBIIX3 perovskites, the band‐gap transition in AI2BB′X6 double perovskites can show substantial metal‐to‐metal charge‐transfer character. This band‐edge orbital composition is used to achieve small band gaps through the selection of energetically aligned B‐ and B′‐site metal frontier orbitals. Calculations reveal a shallow, symmetry‐forbidden region at the band edges for 1, which results in long (μs) microwave conductivity lifetimes. We further describe a facile self‐doping reaction in 2 through Br2 loss at ambient conditions. Kleine Lücke: Anders als in ABX3‐Perowskiten (mit X=Halogenid) hat der Bandlücken‐Übergang in den neuen A2BB′X6‐Doppelperowskiten deutlichen Metall‐Metall‐Ladungstransfer‐Charakter (B zu B′). Somit sind kleine Bandlücken realisierbar, indem die Grenzorbital‐Energien der B‐Metallzentren aufeinander abgestimmt werden; ein Beispiel sind die neuen Doppelperowskite Cs2AgTlX6 (X=Cl und Br).
ISSN:0044-8249
1521-3757
DOI:10.1002/ange.201807421