Related Experiment Video
Updated: Apr 20, 2026

09:39
Characterizing Dissipative Elastic Metamaterials Produced by Additive Manufacturing
Published on: June 28, 2024
1.8K
Wave propagation in bianisotropic metamaterials: angular selective transmission.
Optics Express
|November 18, 2014
Summary
This study explores wave propagation in bianisotropic metamaterials, revealing unique angular selective transmission properties due to asymmetric magnetoelectric tensors. These findings are crucial for developing advanced optical devices.
Area of Science:
- Electromagnetism and Materials Science
- Metamaterials research
- Wave propagation physics
Background:
- Bianisotropic metamaterials exhibit complex electromagnetic responses.
- Asymmetric magnetoelectric tensors with zero diagonal elements define unique material properties.
- Understanding wave propagation is key to metamaterial applications.
Purpose of the Study:
- To investigate wave propagation characteristics in bianisotropic metamaterials.
- To analyze the dispersion relations and eigenwave polarizations.
- To explore angular selective transmission phenomena.
Main Methods:
- Theoretical analysis of wave propagation using a biquadratic dispersion relation.
- Characterization of eigenwaves as elliptically polarized.
- Application of Fourier integral formulation for Gaussian beam incidence.
Main Results:
- Identified two elliptically polarized eigenwaves.
- Observed hybrid elliptic and hyperbolic dispersion characteristics.
- Discovered ordinary and inversion critical angles for angular selective transmission.
Conclusions:
- Bianisotropic metamaterials with specific tensor properties enable angular selective transmission.
- The study provides a theoretical framework for designing metamaterials with tailored optical responses.
- Findings contribute to the development of novel optical components and devices.
More Related Videos
Related Concept Videos
Propagation of Waves
3.4K
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...
3.4K
Interference and Diffraction
55.2K
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.
55.2K
Propagation Speed of Electromagnetic Waves
5.0K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
5.0K
Plane Electromagnetic Waves I
5.4K
The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
The EM field is assumed to be a...
The EM field is assumed to be a...
5.4K
Plane Electromagnetic Waves II
4.4K
Consider a plane wavefront traveling in position x-direction with a constant speed. This wavefront can be utilized to obtain the relationship between electric and magnetic fields with the help of Faraday's law.
4.4K
Magnetostatic Boundary Conditions
1.9K
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
1.9K

