Physics:Quantum Semiconductor physics
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Quantum dots (QDs) or semiconductor nanocrystals are semiconductor particles a few nanometres in size with optical and electronic properties that differ from those of larger particles via quantum mechanical effects. They are a central topic in nanotechnology and materials science.
When a quantum dot is illuminated by ultraviolet light, an electron can be excited from the valence band to the conduction band. The excited electron can then recombine with a hole in the valence band, releasing its energy as light (photoluminescence). The emitted color depends on the energy difference between discrete quantum states.

Introduction
A quantum dot can be defined as a semiconductor structure that confines electrons or holes in all three spatial dimensions, producing discrete energy levels. This confinement resembles a three-dimensional particle in a box model.
Because of this, quantum dots behave similarly to atoms and are often referred to as artificial atoms.[1][2]
The electronic wave functions in quantum dots resemble those in real atoms, reinforcing their atomic-like behavior.[3]
Quantum confinement
The defining property of quantum dots is the quantum confinement effect. As the size of the quantum dot decreases:
- Energy levels become discrete
- The effective band gap increases
- Emission shifts toward shorter wavelengths (blue shift)
Larger quantum dots (≈5–6 nm) emit red/orange light, while smaller dots (≈2–3 nm) emit blue/green light.
The absorption and emission spectra correspond to transitions between quantized energy levels, similar to atomic spectra. This makes quantum dots highly tunable optical materials.
Optical and electronic properties
Quantum dots exhibit properties intermediate between bulk semiconductors and atoms. Their optoelectronic behavior depends strongly on size, shape, and composition.[4]
Key features include:
- Narrow emission spectra
- Size-tunable fluorescence
- High quantum yield
- Discrete energy levels
The emission energy depends on parameters such as:
- Dot size
- Band gap energy
- Effective electron and hole masses
Core–shell and heterostructures
Quantum dots are often engineered as core–shell nanostructures to improve optical performance.
In these systems:
- A semiconductor core is surrounded by a shell with a larger band gap
- Surface defects are passivated
- Non-radiative recombination is reduced
There are four main types:
- Type I
- Inverse Type I
- Type II
- Inverse Type II
Core–shell structures allow tuning of emission wavelength and efficiency. However, lattice mismatch between materials can introduce strain, affecting performance.
Double-shell systems such as CdSe/ZnSe/ZnS improve:
- Fluorescence efficiency
- Stability against photo-oxidation
Surface passivation using ligands (e.g. oleic acid) further enhances stability, though it may reduce photoluminescence efficiency.
Production
Quantum dots can be produced using several methods:
Colloidal synthesis
A solution-based method where precursors decompose to form nanocrystals. Growth is controlled by temperature and monomer concentration.
This method enables:
- Precise size control
- Large-scale production
- Monodisperse particles
Common materials include:
- CdSe, CdS, PbS, PbSe
- InAs, InP
- Perovskite quantum dots
Plasma synthesis
A gas-phase method allowing control of size, composition, and doping.
Self-assembly
Quantum dots can form spontaneously due to lattice mismatch during epitaxial growth (Stranski–Krastanov mode).
Lithographic fabrication
Quantum dots can be defined using nanofabrication techniques and gate electrodes in semiconductor devices.
Applications
Quantum dots are widely used due to their tunable properties:
- LEDs and displays (QLED technology)
- solar cells
- quantum computing and qubits
- single-electron transistors
- lasers and single-photon sources
- medical imaging and biological labeling
Their ability to emit specific wavelengths makes them ideal for high-color-accuracy displays and optical devices.
Optical properties
Quantum dots have highly tunable optical behavior due to confinement of excitons.
An exciton consists of:
- An excited electron
- A hole in the valence band
These are bound by Coulomb interaction. When the dot size approaches the exciton Bohr radius, confinement increases the band gap energy.
As a result:
- Smaller dots → higher energy emission
- Larger dots → lower energy emission
Fluorescence lifetime also depends on size, with larger dots showing longer lifetimes.
Health and safety
Some quantum dots, particularly those containing cadmium, may pose health and environmental risks.
Toxicity depends on:
- Size and composition
- Surface chemistry
- Environmental conditions
Under certain conditions (e.g. UV exposure), quantum dots can release toxic ions or generate reactive oxygen species.
Research continues into safer alternatives such as:
- Carbon quantum dots
- Cadmium-free nanocrystals
See also
Table of contents (138 articles)
Index
Full contents
- Physics:Quantum Interpretations of quantum mechanics
- Physics:Quantum Wave–particle duality
- Physics:Quantum Complementarity principle
- Physics:Quantum Uncertainty principle
- Physics:Quantum Measurement problem
- Physics:Quantum Bell's theorem
- Physics:Quantum Hidden variable theory
- Physics:Quantum A Spooky Action at a Distance
- Physics:Quantum A Walk Through the Universe
- Physics:Quantum The Secret of Cohesion and How Waves Hold Matter Together

- Physics:Quantum Density matrix
- Physics:Quantum Exactly solvable quantum systems
- Physics:Quantum Formulas Collection
- Physics:Quantum A Matter Of Size
- Physics:Quantum Symmetry in quantum mechanics
- Physics:Quantum Angular momentum operator
- Physics:Quantum Runge–Lenz vector
- Physics:Quantum Approximation Methods
- Physics:Quantum Matter Elements and Particles
- Physics:Quantum Dirac equation
- Physics:Quantum Klein–Gordon equation

- Physics:Quantum Atomic structure and spectroscopy
- Physics:Quantum Hydrogen atom
- Physics:Quantum Multi-electron atoms
- Physics:Quantum Fine structure
- Physics:Quantum Hyperfine structure
- Physics:Quantum Isotopic shift
- Physics:Quantum Zeeman effect
- Physics:Quantum Stark effect
- Physics:Quantum Spectral lines and series
- Physics:Quantum Selection rules
- Physics:Quantum Fermi's golden rule

- Physics:Quantum Wavefunction
- Physics:Quantum Superposition principle
- Physics:Quantum Eigenstates and eigenvalues
- Physics:Quantum Boundary conditions and quantization
- Physics:Quantum Standing waves and modes
- Physics:Quantum Normal modes and field quantization
- Physics:Number of independent spatial modes in a spherical volume
- Physics:Quantum Density of states

- Physics:Quantum Time evolution
- Physics:Quantum Schrödinger equation
- Physics:Quantum Time-dependent Schrödinger equation
- Physics:Quantum Stationary states
- Physics:Quantum Perturbation theory
- Physics:Quantum Time-dependent perturbation theory
- Physics:Quantum Adiabatic theorem
- Physics:Quantum Scattering theory
- Physics:Quantum S-matrix

- Physics:Quantum Nonlinear King plot anomaly in calcium isotope spectroscopy
- Physics:Quantum optics beam splitter experiments
- Physics:Quantum Ultra fast lasers
- Physics:Quantum Experimental quantum physics Template:Quantum optics operators

- Physics:Quantum field theory (QFT) basics
- Physics:Quantum field theory (QFT) core
- Physics:Quantum Fields and Particles
- Physics:Quantum Second quantization
- Physics:Quantum Harmonic Oscillator field modes
- Physics:Quantum Creation and annihilation operators
- Physics:Quantum vacuum fluctuations
- Physics:Quantum Propagators in quantum field theory
- Physics:Quantum Feynman diagrams
- Physics:Quantum Path integral formulation
- Physics:Quantum Renormalization in field theory
- Physics:Quantum Renormalization group
- Physics:Quantum Field Theory Gauge symmetry
- Physics:Quantum Non-Abelian gauge theory
- Physics:Quantum Electrodynamics (QED)
- Physics:Quantum chromodynamics (QCD)
- Physics:Quantum Electroweak theory
- Physics:Quantum Standard Model

- Physics:Quantum Statistical mechanics
- Physics:Quantum Partition function
- Physics:Quantum Distribution functions
- Physics:Quantum Liouville equation
- Physics:Quantum Kinetic theory
- Physics:Quantum Boltzmann equation
- Physics:Quantum BBGKY hierarchy
- Physics:Quantum Transport theory
- Physics:Quantum Relaxation and thermalization
- Physics:Quantum Thermodynamics

- Physics:Quantum Plasma (fusion context)
- Physics:Quantum Fusion reactions and Lawson criterion
- Physics:Quantum Magnetic confinement fusion
- Physics:Quantum Inertial confinement fusion
- Physics:Quantum Plasma instabilities and turbulence
- Physics:Quantum Tokamak
- Physics:Quantum Tokamak core plasma
- Physics:Quantum Tokamak edge physics and recycling asymmetries
- Physics:Quantum Stellarator

- Physics:Quantum mechanics/Timeline
- Physics:Quantum mechanics/Timeline/Pre-quantum era
- Physics:Quantum mechanics/Timeline/Old quantum theory
- Physics:Quantum mechanics/Timeline/Modern quantum mechanics
- Physics:Quantum mechanics/Timeline/Quantum field theory era
- Physics:Quantum mechanics/Timeline/Quantum information era
- Physics:Quantum mechanics/Timeline/Quantum technology era
- Physics:Quantum mechanics/Timeline/Quiz/

References
- ↑ Silbey, Robert J.; Alberty, Robert A.; Bawendi, Moungi G. (2005). Physical Chemistry (4th ed.). John Wiley & Sons. p. 835.
- ↑ Ashoori, R. C. (1996). "Electrons in artificial atoms". Nature 379: 413–419. doi:10.1038/379413a0.
- ↑ Banin, Uri; Cao, YunWei; Katz, David; Millo, Oded (1999). "Identification of atomic-like electronic states in indium arsenide nanocrystal quantum dots". Nature 400: 542–544.
- ↑ Murray, C. B.; Kagan, C. R.; Bawendi, M. G. (2000). "Synthesis and Characterization of Monodisperse Nanocrystals". Annual Review of Materials Research 30: 545–610.






