Related Experiment Video
Updated: May 4, 2026

12:19
Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
Published on: April 4, 2017
7.9K
A semiconductor source of triggered entangled photon pairs.
R M Stevenson1, R J Young, P Atkinson
1Toshiba Research Europe Limited, 260 Cambridge Science Park, Cambridge CB4 0WE, UK.
Nature
|January 13, 2006
Summary
Researchers demonstrate triggered polarization-entangled photon pairs from quantum dots by tuning exciton energy splitting to zero. This breakthrough offers a promising path toward on-demand entangled photon sources for quantum information applications.
Area of Science:
- Quantum Optics
- Solid-State Physics
- Quantum Information Science
Background:
- Entangled photon pairs are crucial for quantum information technologies like quantum key distribution.
- Quantum dots decaying from biexcitons are a proposed source of entangled photons.
- Previous experiments showed classical correlations due to exciton energy splitting.
Purpose of the Study:
- To demonstrate triggered polarization-entangled photon pair emission from single quantum dots.
- To overcome limitations of previous methods that resulted in classical correlations.
- To enable on-demand generation of entangled photons for quantum applications.
Main Methods:
- Utilizing biexciton radiative decay in single quantum dots.
- Tuning the intermediate exciton energy splitting to zero.
- Employing an in-plane magnetic field or precise control of growth conditions.
Main Results:
- Achieved triggered photon pair emission from quantum dots.
- Demonstrated emission characteristics suggestive of polarization entanglement.
- Successfully eliminated classical correlations by minimizing exciton energy splitting.
Conclusions:
- On-demand generation of polarization-entangled photon pairs from quantum dots is feasible.
- This method overcomes drawbacks of other entanglement schemes, such as multiple pair emission.
- A simple semiconductor light-emitting diode could potentially host a triggered entangled photon pair source.
Related Concept Videos
Photoluminescence: Applications
1.3K
Photoluminescence offers a wide range of applications due to its inherent sensitivity and selectivity. This technique allows for both direct and indirect analyses of the analyte. Direct quantitative analysis is possible when the analyte exhibits a favorable quantum yield for fluorescence or phosphorescence. However, an indirect analysis may be feasible if the analyte is not fluorescent or phosphorescent, or if the quantum yield is unfavorable. Indirect methods include reacting the analyte with...
1.3K
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
Carrier Generation and Recombination
1.5K
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...
1.5K

