Related Experiment Video
Updated: Apr 15, 2026

07:42
Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
Published on: December 15, 2021
3.6K
Diffraction-induced instability of coupled dark solitary waves
Optics Letters
|April 15, 2015
Summary
Coupled dark solitons with different wavelengths become unstable, causing the stronger diffracting component to radiate. This leaves a single dark soliton, demonstrating a novel instability in nonlinear optics.
Area of Science:
- Nonlinear Optics
- Soliton Dynamics
- Wave Propagation
Background:
- Coupled dark solitary beams are described by coupled defocusing nonlinear Schrödinger equations.
- Vector dark solitons can exist on backgrounds with different wavelengths and diffraction coefficients.
Purpose of the Study:
- To investigate a novel instability in the propagation of coupled dark solitary beams.
- To understand the behavior of vector dark solitons with differing diffraction properties.
Main Methods:
- Theoretical analysis using perturbation theory.
- Numerical integration of the governing coupled defocusing nonlinear Schrödinger equations.
Main Results:
- The vector dark soliton solution is found to be unstable to radiation modes.
- The component with stronger diffraction radiates energy away.
- A single dark soliton remains in the less diffracting mode/wavelength.
Conclusions:
- A novel instability mechanism for coupled dark solitons is identified.
- Differential diffraction significantly impacts the stability and evolution of vector dark solitons.
- This instability leads to the decay of vector solitons into stable single solitons.
Related Concept Videos
Interference and Diffraction
54.8K
Interference is a characteristic phenomenon exhibited by waves. When two electromagnetic waves interact with their peaks and troughs coinciding, a resulting wave with enhanced amplitude is produced. This is known as constructive interference. In this case, the two waves interacting are in phase with each other.
54.8K
Microtubule Instability
6.5K
Microtubules are hollow cylindrical filaments having a diameter of approximately 25 nm and a length that varies from 200 nm to 25 μm. GTP-bound tubulin subunits form αβ-heterodimers for microtubule assembly. These core building blocks interact longitudinally, polymerizing into protofilaments. The protofilaments then interact with one another through lateral bonding forces to form stable cylindrical microtubules. These cylindrical filaments are dynamic as they undergo repeated...
6.5K
Microtubule Instability
6.3K
6.3K
Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model
924
Various dissolution theories provide insight into the factors that influence the dissolution rate. Danckwerts' Model suggests that turbulence, rather than a stagnant layer, characterizes the dissolution medium at the solid-liquid interface. In this model, the agitated solvent contains macroscopic packets that move to the interface via eddy currents, facilitating the absorption and delivery of the drug to the bulk solution. The regular replenishment of solvent packets maintains the...
924
Theories of Dissolution: Diffusion Layer Model
2.3K
Dissolution, the process by which drug particles dissolve in a solvent, is explained by the diffusion layer model, a theoretical framework that simulates the absorption of oral drugs and allows us to analyze experimental data.
This process starts with a thin layer, saturated with the drug, forming at the interface between the solid and liquid. The solute then diffuses from this layer into the main solution. The Noyes-Whitney equation suggests that the rate of dissolution relies on the diffusion...
This process starts with a thin layer, saturated with the drug, forming at the interface between the solid and liquid. The solute then diffuses from this layer into the main solution. The Noyes-Whitney equation suggests that the rate of dissolution relies on the diffusion...
2.3K
Carrier Generation and Recombination
1.6K
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...
1.6K

