Related Experiment Video
Updated: Jan 16, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
Anomalous Metallic Cubic CsCuBr3 Perovskites: Pressure- and Temperature-Driven Suppression of Jahn-Teller Distortion
Mei Li1, Pengfei Shan2, Bohao Zhao1
1Center for High Pressure Science and Technology Advanced Research (HPSTAR), Beijing 100193, China.
Abstract:
Distinct from traditional halide perovskites, which are based on main-group elements (e.g., Pb2+, Sn2+, Ge2+) and are typically semiconducting, transition metals like Cu2+─characterized by partially filled d-orbitals─offer unique advantages in modulating the electronic behavior of perovskite materials. However, the strong Jahn-Teller effect of Cu2+ makes it a significant challenge for stabilizing a robust three-dimensional perovskite framework. Herein, we report the first synthesis of a metallic cubic perovskite phase of CsCuBr3 via a tailored structural design under high-temperature and high-pressure conditions. In situ synchrotron X-ray diffraction reveals that the orthorhombic nonperovskite CsCuBr3 precursor (space group C2221) transforms into a cubic perovskite structure (space group Pm-3m) featuring an undistorted corner-sharing octahedral framework at ∼22 GPa and ∼603 K. The perovskite structure remains stable at pressure down to 4.3 GPa at room temperature, while at low temperatures below 50 K, it may be recovered to ambient pressure. Notably, the structure lacks both the expected luminescence and a distinct absorption edge, instead exhibiting a metallic behavior, as confirmed by temperature-dependent resistance measurements. Electronic structure calculations at 22.4 GPa and 0 K further reveal pronounced hybridization between the Cu-3d and Br-4p orbitals near the Fermi level, leading to an enhanced orbital degeneracy and electron delocalization. These findings demonstrate that the lattice contraction effectively suppresses the strong Jahn-Teller distortion intrinsic to Cu2+, offering a promising strategy for the design of high-performance novel materials.
More Related Videos
08:42High-Sensitivity Nuclear Magnetic Resonance at Giga-Pascal Pressures: A New Tool for Probing Electronic and Chemical Properties of Condensed Matter under Extreme Conditions
Published on: October 10, 2014
08:55Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses
Published on: June 7, 2018
Related Concept Videos
Crystal Field Theory - Octahedral Complexes
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
Theory of Metallic Conduction
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
Temperature Dependent Deformation
Atomic Spectroscopy: Effects of Temperature
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...