Efficient Direct Band-Gap Transition in Germanium by Three-Dimensional Strain.
Simon Mellaerts1, Valeri Afanas'ev1, Jin Won Seo2
1Department of Physics and Astronomy, KU Leuven, Celestijnenlaan 200D, 3001 Leuven, Belgium.
ACS Applied Materials & Interfaces
|June 22, 2021
Summary
Applying 3D strain to germanium (Ge) can create a direct band gap, enhancing optical and transport properties. This computational study reveals potential for optimizing semiconductor materials through controlled deformation.
Area of Science:
- Materials Science and Engineering
- Condensed Matter Physics
- Semiconductor Device Physics
Background:
- Advancements in three-dimensional (3D) integrated circuits necessitate novel strategies for enhancing device performance.
- Exploring material properties under deformation is crucial for developing next-generation electronic components.
- Computational predictive methods are essential for identifying optimal strain conditions.
Purpose of the Study:
- To investigate the effects of isotropic 3D strain on the properties of germanium (Ge) using first-principles calculations.
- To identify specific strain tensors that yield desired electronic and optical characteristics in Ge.
- To explore the potential of 3D deformation in optimizing semiconductor materials.
Main Methods:
- Utilized first-principles calculations to model germanium (Ge) under isotropic 3D strain.
- Employed the Boltzmann transport equation for simulating charge transport properties.
- Applied the many-body Bethe-Salpeter equation (BSE) for analyzing optical properties.
Main Results:
- Achieved a direct band gap in Ge with only 0.70% triaxial tensile strain, bypassing challenges of tin (Sn) doping.
- Observed significant enhancements in refractive index and carrier mobility, especially for electrons.
- Demonstrated the feasibility of realizing desirable material properties through precise 3D strain engineering.
Conclusions:
- 3D strain engineering is a powerful approach for tuning semiconductor properties, offering an alternative to chemical doping.
- Germanium under specific triaxial tensile strain exhibits improved electronic and optical characteristics.
- The study highlights the broad potential of exploring the 3D deformation space for optimizing various materials.
Related Concept Videos
Carrier Generation and Recombination
908
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
908
Semiconductors
1.0K
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...
1.0K
Fermi Level Dynamics
421
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...
421
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
Metal-Semiconductor Junctions
603
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...
603
Biasing of Metal-Semiconductor Junctions
403
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
403


