Pressure Effects on Structure and Optical Properties in Cesium Lead Bromide Perovskite Nanocrystals.

Title Pressure Effects on Structure and Optical Properties in Cesium Lead Bromide Perovskite Nanocrystals.
Authors G. Xiao; Y. Cao; G. Qi; L. Wang; C. Liu; Z. Ma; X. Yang; Y. Sui; W. Zheng; B. Zou
Journal J Am Chem Soc
DOI 10.1021/jacs.7b05260
Abstract

Metal halide perovskites (MHPs) are gaining increasing interest because of their extraordinary performance in optoelectronic devices and solar cells. However, developing an effective strategy for achieving the bandgap engineering of MHPs that will satisfy the practical applications remains a great challenge. In this study, high pressure is introduced to tailor the optical and structural properties of MHP-based cesium lead bromide nanocrystals (CsPbBr3 NCs), which exhibit excellent thermodynamic stability. Both the pressure-dependent steady-state photoluminescence and absorption spectra experience a stark discontinuity at ~1.2 GPa, where an isostructural phase transformation regarding Pbnm space group occurs. The physical origin points to the repulsive force impact due to the overlap between the valence electron charge clouds of neighboring layers. Simultaneous bandgap narrowing and carrier-lifetime prolongation of CsPbBr3 trihalide pe-rovskite NCs were also achieved as expected, which facilitates the broader solar spectrum absorption for photovoltaic applications. Note that the values of phase change interval and bandgap redshift of CsPbBr3 nanowires are between the ones for CsPbBr3 nanocubes and the corresponding bulk counterparts, which results from the unique geometrical mor-phology effect. First-principles calculations unravel that the bandgap engineering is governed by orbital interactions with-in inorganic Pb-Br frame through structural modification. Changes of band structures are attributed to the synergistic effect of pressure-induced modulations of Br-Pb bond length and Pb-Br-Pb bond angle for PbBr6 octahedral framework. Furthermore, the significant distortion of lead-bromide octahedron to accommodate the Jahn-Teller effect at much high-er pressure would eventually lead to a direct to indirect bandgap electronic transition. This study enables high pressure as a robust tool to control the structure and bandgap of CsPbBr3 NCs, and thus providing an insight into the microscopic physiochemical mechanism of those compressed MHP nanosystems.

Citation G. Xiao; Y. Cao; G. Qi; L. Wang; C. Liu; Z. Ma; X. Yang; Y. Sui; W. Zheng; B. Zou.Pressure Effects on Structure and Optical Properties in Cesium Lead Bromide Perovskite Nanocrystals.. J Am Chem Soc. 2017. doi:10.1021/jacs.7b05260

Related Elements

Cesium

See more Cesium products. Cesium (or Caesium) (atomic symbol: Ce, atomic number: 55) is a Block S, Group 1, Period 6 element with an atomic weight of 132.9054519. The number of electrons in each of Cesium's shells is 2, 8, 18, 18, 8, 1 and its electron configuration is [Xe]6s1. Cesium Bohr ModelThe cesium atom has a radius of 265 pm and a Van der Waals radius of 343 pm. Cesium is a member of the alkali group of metals. It is one of three metals that occur as a liquid at room temperature, the others being mercury and gallium. Elemental CesiumCesium's main commercial source is pollucite ore; however, it is also found in beryl, avogadrite, pezzottaite, and londonite. Cesium was discovered by Robert Bunsen and Gustav Kirchhoff in 1860 and first isolated by Carl Setterberg in 1882. In its elemental form, cesium has a silvery gold appearance. The word Cesium originates from the Latin word "caesius," meaning "sky blue," which refers to the vibrant blue lines in its spectrum.

Bromine

See more Bromine products. Bromine (atomic symbol: Br, atomic number: 35) is a Block P, Group 17, Period 4 element. Its electron configuration is [Ar]4s23d104p5. The bromine atom has a radius of 102 pm and its Van der Waals radius is 183 pm. In its elemental form, bromine Bromine Bohr Model has a red-brown appearance. Bromine does not occur by itself in nature; it is found as colorless soluble crystalline mineral halide salts. Bromine was discovered and first isolated by Antoine Jérôme Balard and Leopold Gmelin in 1825-1826.

Lead

Lead Bohr ModelSee more Lead products. Lead (atomic symbol: Pb, atomic number: 82) is a Block P, Group 14, Period 6 element with an atomic radius of 207.2. The number of electrons in each of Lead's shells is [2, 8, 18, 32, 18, 4] and its electron configuration is [Xe] 4f14 5d10 6s2 6p2. The lead atom has a radius of 175 pm and a Van der Waals radius of 202 pm. In its elemental form, lead has a metallic gray appearance. Lead occurs naturally as a mixture of four stable isotopes: 204Pb (1.48%), 206Pb (23.6%), 207Pb (22.6%), and 208Pb (52.3%). Elemental LeadLead is obtained mainly from galena (PbS) by a roasting process. Anglesite, cerussite, and minim are other common lead containing minerals. Lead does occur as a free element in nature, but it is rare. It is a dense, soft metal that is very resistant to corrosion and poorly conductive compared to other metals. Its density and low melting point make it useful in applications such as electrolysis and industrial materials.

Related Forms & Applications