Related Experiment Video
Updated: Mar 29, 2026

08:12
Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films
Published on: September 8, 2017
10.2K
Relation between bandgap and resistance drift in amorphous phase change materials
Martin Rütten1,2, Matthias Kaes1, Andreas Albert1
1Institute of Physics 1A, RWTH Aachen University, Sommerfeldstrasse 14, 52074 Aachen, Germany.
Scientific Reports
|December 2, 2015
Summary
Phase change materials offer fast memory but suffer resistance drift. New research shows Ag4In3Sb67Te26 has reduced drift, paving the way for improved multilevel storage devices.
Area of Science:
- Materials Science
- Solid State Physics
- Device Engineering
Background:
- Phase change materials are key for next-generation memory, bridging storage and memory access times.
- Resistance drift in amorphous phase change materials hinders multilevel storage capabilities.
- Understanding structural relaxation is crucial for mitigating drift.
Purpose of the Study:
- To investigate the temporal evolution of optical properties in amorphous phase change materials.
- To analyze the relationship between bandgap widening, dielectric constant, and activation energy.
- To identify phase change materials with reduced resistance drift.
Main Methods:
- Temporal evolution of infrared spectra measured on amorphous thin films.
- Analysis of Ag4In3Sb67Te26, GeTe, and Ge2Sb2Te5.
- Quantitative comparison with experimental data for activation energy.
Main Results:
- Annealing causes bandgap widening and decreased optical dielectric constant (ε∞) in all studied materials.
- Temporal evolution of bandgap and activation energy can be decoupled.
- Ag4In3Sb67Te26 exhibits a smaller increase in activation energy compared to bandgap widening, indicating reduced resistance drift.
Conclusions:
- Decoupling of bandgap and activation energy evolution offers a pathway to design materials with suppressed resistance drift.
- Ag4In3Sb67Te26 presents a promising candidate for phase change memory with enhanced multilevel storage stability.
- This study provides insights for developing novel phase change materials with improved performance.
More Related Videos
Related Concept Videos
Semiconductors
1.9K
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...
1.9K
Energy Bands in Solids
2.4K
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...
2.4K
Band Theory
17.8K
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,...
17.8K
Theory of Metallic Conduction
1.9K
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the 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,...
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,...
1.9K
Fermi Level Dynamics
976
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
976
Metal-Semiconductor Junctions
1.3K
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
1.3K

