Related Experiment Video
Updated: Mar 14, 2026

10:40
High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
Published on: June 28, 2016
8.0K
Surface Chemistry of Semiconducting Quantum Dots: Theoretical Perspectives
Svetlana V Kilina1, Patrick K Tamukong1, Dmitri S Kilin1
1Department of Chemistry and Biochemistry, North Dakota State University , Fargo, North Dakota 58108, United States.
Accounts of Chemical Research
|September 27, 2016
Summary
Computational modeling reveals how surface passivation and ligands impact colloidal quantum dots (QDs) for energy and lighting. Understanding these effects is key to optimizing QD photophysics and performance.
Area of Science:
- Materials Science
- Quantum Chemistry
- Nanotechnology
Background:
- Colloidal quantum dots (QDs) are promising for energy and lighting but highly sensitive to surface defects and passivation.
- Direct measurement of surface states is challenging, necessitating computational approaches for understanding photophysics.
- The role of passivating ligands in QD photodynamics requires further elucidation.
Purpose of the Study:
- To review computational methods for understanding surface effects on QD photophysics.
- To discuss recent progress in modeling surface passivation and its impact on light-driven processes in QDs.
- To explain experimental trends in CdSe, PbSe, and Si QDs using quantum-chemical calculations.
Main Methods:
- Effective Mass Approximation (EMA) for large QDs.
- Time-Dependent Density Functional Theory (TDDFT) for smaller QDs and surface effects.
- Multiconfiguration approaches for highly correlated electronic states and extrapolation to larger QDs.
- Nonadiabatic dynamics (NAD) with surface hopping (SH) for light-driven processes.
Main Results:
- EMA accurately predicts optical properties of large CdSe QDs; TDDFT is crucial for smaller QDs where surface effects dominate.
- Calculations confirm efficient two-photon absorption in QDs, enabling nonlinear optical applications.
- Ligand type significantly influences QD emission; anionic ligands can eliminate midgap states in nonstoichiometric QDs, improving luminescence.
Conclusions:
- Computational modeling provides critical insights into surface passivation and ligand effects on QD photophysics.
- Surface engineering via ligand choice and stoichiometry control is vital for optimizing QD performance in energy and lighting applications.
- Advanced methods like TDDFT and NAD are essential for explaining and predicting QD behavior, guiding future material design.
Related Concept Videos
Semiconductors
1.8K
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...
1.8K
Metal-Semiconductor Junctions
1.2K
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...
1.2K
Fermi Level Dynamics
914
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...
914
Types of Semiconductors
1.7K
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...
1.7K
Valence Bond Theory
11.5K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
11.5K
Energy Bands in Solids
2.2K
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...
2.2K

