Related Experiment Video
Updated: Mar 22, 2026

09:43
Transmission of Multiple Signals through an Optical Fiber Using Wavefront Shaping
Published on: March 20, 2017
10.4K
Radiating dispersive shock waves in non-local optical media
1Department of Mathematical Sciences , Loughborough University , Loughborough LE11 3TU, UK.
Summary
We studied nonlinear wave propagation in liquid crystals. A novel dispersive shock wave (DSW) with positive polarity was discovered, generating leading resonant radiation and exhibiting classical shock velocity.
Area of Science:
- Nonlinear Optics
- Condensed Matter Physics
- Fluid Dynamics
Background:
- Coherent light beam propagation in nematic liquid crystals follows a defocusing nonlinear Schrödinger (NLS) equation.
- Dispersive shock waves (DSWs) are a known phenomenon in nonlinear wave propagation.
- Standard DSW solutions of the defocusing NLS equation exhibit specific characteristics.
Purpose of the Study:
- To analyze the step Riemann problem for light beam propagation in nematic liquid crystals.
- To investigate the unique properties of the DSW generated in this system.
- To develop an asymptotic theory for the nematic DSW and compare it with numerical simulations.
Main Methods:
- Analysis of the step Riemann problem for the governing nonlinear wave equations.
- Application of the Wentzel-Kramers-Brillouin (WKB) approximation to find the radiative wavetrain solution.
- Derivation of an asymptotic model using a Korteweg-de Vries equation with fifth-order dispersion.
- Direct numerical simulations for validation.
Main Results:
- The generated DSW exhibits positive polarity, differing from standard NLS DSWs.
- The DSW generates resonant radiation that propagates ahead of the wave.
- The velocity of the leading soliton of the DSW is determined by the classical shock velocity.
- The asymptotic theory, a fifth-order dispersive Korteweg-de Vries equation, accurately describes the radiation generation.
Conclusions:
- The nematic liquid crystal system generates a unique DSW with distinct properties.
- Resonant radiation ahead of the DSW is a key feature, explained by the derived asymptotic model.
- The study provides a theoretical framework and numerical validation for this nonlinear wave phenomenon.
More Related Videos
Related Concept Videos
Shock Waves
2.7K
While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...
2.7K
Propagation of Waves
3.2K
When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
3.2K
Standing Waves in a Cavity
1.6K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.6K
Electromagnetic Waves in Matter
4.2K
Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore,...
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore,...
4.2K
Propagation Speed of Electromagnetic Waves
4.9K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
4.9K
Interference and Diffraction
53.8K
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.
53.8K

