Related Experiment Video
Updated: Jul 22, 2026

11:07
Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties
Published on: August 15, 2015
9.9K
A first-principles study: single-layer TiS2 modified by non-metal doping.
Shu Chen1, Lu Yang2, Jinlin Bao1
1Shenyang University of Technology, Shenyang, 110870, China.
Journal of Molecular Modeling
|December 1, 2022
Summary
Nonmetal doping of titanium disulfide (TiS2) with elements like boron, carbon, nitrogen, oxygen, and phosphorus significantly alters its electronic structure and band gap. This study reveals how doping impacts TiS2 stability and bonding mechanisms.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Computational Chemistry
Background:
- Monolayer TiS2 is a promising material with tunable electronic properties.
- Understanding the impact of doping is crucial for optimizing its applications.
Purpose of the Study:
- To investigate the effects of substitutional nonmetal doping (B, C, N, O, P) on the electronic structure of monolayer TiS2.
- To analyze the mechanism of band gap modification and system stability upon doping.
Main Methods:
- First-principles calculations were employed to study the electronic structure.
- Analysis included stability, charge transfer, electron cloud overlap population, and formation energy.
- Density of States (DOS) and charge density difference were used to understand bonding.
Main Results:
- Doping confirmed the stability of the TiS2 system with varying Ti-X bond distortions.
- Boron, carbon, and nitrogen doping showed concentration-dependent property changes.
- Oxygen doping led to a gradual band gap expansion with increasing doping rate.
Conclusions:
- Nonmetal doping effectively modifies the electronic structure and band gap of monolayer TiS2.
- The study elucidates the interaction mechanisms and bonding processes between dopants and the TiS2 lattice.
Related Concept Videos
Metallic Solids
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability. Many...
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability. Many...
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Tetrahedral 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,...
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,...
Types of Semiconductors
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
Metal-Semiconductor Junctions
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 semiconductor's...
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 semiconductor's...
Biasing of Metal-Semiconductor Junctions
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...

