Related Experiment Video
Updated: Nov 2, 2025

07:56
A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
Published on: September 5, 2019
8.7K
Spectrally pure photon pair generation in asymmetric heterogeneously coupled waveguides
Optics Letters
|June 15, 2021
Summary
Researchers developed a new method for creating spectrally pure photon pairs using asymmetric coupled waveguides. This technique enables precise control over light properties for advanced quantum applications.
Area of Science:
- Quantum optics
- Integrated photonics
- Materials science
Background:
- Generating spectrally pure photon pairs is crucial for quantum information processing.
- Conventional methods often face limitations due to material dispersion.
Purpose of the Study:
- To develop a design methodology for generating spectrally pure photon pairs in asymmetric heterogeneously coupled waveguides.
- To overcome limitations imposed by material dispersion for group velocity matching.
Main Methods:
- Utilizing spontaneous parametric down-conversion (SPDC) in asymmetric coupled waveguides.
- Employing mode coupling to tailor supermode group velocities.
- Designing based on thin-film lithium niobate waveguides.
Main Results:
- Achieved group velocity matching not possible through material dispersion alone.
- Demonstrated high spectral purity of generated photon pairs.
- Showcased temperature tunability of the waveguide system.
Conclusions:
- The proposed design methodology offers a versatile strategy for single-photon source development.
- Applicable to various waveguide materials and structures.
- Enables enhanced control over photon pair properties for quantum technologies.
Related Concept Videos
Generating Electromagnetic Radiations
5.2K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
5.2K
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
IR Spectrum Peak Splitting: Symmetric vs Asymmetric Vibrations
1.4K
Identical bonds within a polyatomic group can stretch symmetrically (in-phase) or asymmetrically (out-of-phase). Similar to hydrogen bonding, these vibrations also influence the shape of the IR peak. Generally, asymmetric stretching frequencies are higher than symmetric stretching frequencies. For example, primary amines exhibit two distinct IR peaks between 3300–3500 cm−1 corresponding to the symmetric and asymmetric N-H stretching, while secondary amines exhibit a single...
1.4K
The de Broglie Wavelength
31.1K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
31.1K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
1.2K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.2K

