Related Experiment Video
Updated: Nov 9, 2025

08:12
Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films
Published on: September 8, 2017
9.8K
Accessing the Conduction Band Dispersion in CH3NH3PbI3 Single Crystals
Jinpeng Yang1,2, Haruki Sato3, Hibiki Orio3
1College of Physical Science and Technology, Yangzhou University, Jiangsu, China.
The Journal of Physical Chemistry Letters
|April 12, 2021
Summary
Researchers studied methylammonium lead iodide (CH3NH3PbI3) using AR-2PPE and AR-LEIPS. They observed conduction band dispersion and determined the electron effective mass, consistent with cubic phase calculations.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Solid-State Chemistry
Background:
- Methylammonium lead iodide (CH3NH3PbI3) is a key material in perovskite solar cells.
- Understanding its electronic band structure is crucial for optimizing device performance.
- Previous studies have faced challenges in characterizing its conduction band properties.
Purpose of the Study:
- To investigate the conduction band dispersion in CH3NH3PbI3.
- To determine the electron effective mass at the Γ point.
- To explore the temperature-dependent electronic properties and surface effects.
Main Methods:
- Angle-resolved two-photon photoelectron spectroscopy (AR-2PPE) with low photon intensity.
- Angle-resolved low-energy inverse photoelectron spectroscopy (AR-LEIPS).
Main Results:
- Clear conduction band energy dispersion along the Γ-M direction was observed using both AR-2PPE and AR-LEIPS.
- The experimental results are consistent with theoretical band calculations for the cubic phase.
- The electron effective mass at the Γ point was determined to be (0.20 ± 0.05)m0 at 90 K.
- Discrepancies in observed conduction band energy were attributed to electronic correlation effects in probing initial and final states.
Conclusions:
- The study provides the first direct observation of conduction band dispersion in CH3NH3PbI3 using independent spectroscopic methods.
- The findings confirm the cubic-phase electronic properties of CH3NH3PbI3, even at lower temperatures, suggesting surface-dominated electronic behavior.
- The results offer valuable insights into the fundamental electronic properties of methylammonium lead iodide for optoelectronic applications.
More Related Videos
Related Concept Videos
Energy Bands in Solids
1.5K
Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
1.5K
Band Theory
16.3K
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
16.3K
Semiconductors
1.1K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.1K

