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Halide Perovskites: Advanced Photovoltaic Materials Empowered by a Unique Bonding Mechanism

Matthias Wuttig, Carl‐Friedrich Schön, Mathias Schumacher, John Robertson, Pavlo Golub, Éric Bousquet, Carlo Gatti, Jean‐Yves Raty

2021Advanced Functional Materials106 citationsDOIOpen Access PDF

Abstract

Abstract Outstanding photovoltaic (PV) materials combine a set of advantageous properties including large optical absorption and high charge carrier mobility, facilitated by small effective masses. Halide perovskites (ABX 3 , where X = I, Br, or Cl) are among the most promising PV materials. Their optoelectronic properties are governed by the BX bond, which is responsible for the pronounced optical absorption and the small effective masses of the charge carriers. These properties are frequently attributed to the n s 2 configuration of the B atom, i.e., Pb 6s 2 or Sn 5s 2 (“lone‐pair”) states. The analysis of the PV properties in conjunction with a quantum‐chemical bond analysis reveals a different scenario. The BX bond differs significantly from ionic, metallic, or conventional 2c2e covalent bonds. Instead it is better regarded as metavalent, since it shares about one p‐electron between adjacent atoms. The resulting σ‐bond, formally a 2c1e bond, is half‐filled, causing pronounced optical absorption. Electron transfer between B and X atoms and lattice distortions open a moderate bandgap resulting in charge carriers with small effective masses. Hence, metavalent bonding explains favorable PV properties of halide perovskites, as summarized in a map for different bond types, which provides a blueprint to design PV materials.

Topics & Concepts

Materials scienceIonic bondingCovalent bondBand gapHalideCharge carrierLone pairAbsorption (acoustics)Chemical physicsOptoelectronicsInorganic chemistryMoleculeIonChemistryComposite materialOrganic chemistryPerovskite Materials and ApplicationsThermal Expansion and Ionic ConductivityChalcogenide Semiconductor Thin Films