Related Experiment Video
Updated: Apr 15, 2026

13:44
Simulation, Fabrication and Characterization of THz Metamaterial Absorbers
Published on: December 27, 2012
16.0K
One-way absorber for linearly polarized electromagnetic wave utilizing composite metamaterial
Optics Express
|April 4, 2015
Summary
This study introduces a novel one-way absorber for linearly polarized electromagnetic waves. This device selectively absorbs waves in one direction while transmitting them in the opposite, enabling asymmetric transmission applications.
Area of Science:
- Metamaterials
- Electromagnetics
- Wave Propagation
Background:
- Metamaterials offer unique electromagnetic properties.
- Controlling wave propagation direction and polarization is crucial for advanced devices.
- Asymmetric transmission of electromagnetic waves is a key challenge.
Purpose of the Study:
- To propose and design a one-way absorber for selective linearly polarized electromagnetic waves.
- To combine polarization rotation with polarization-selective absorption using composite metamaterials.
- To achieve directional control over electromagnetic wave propagation.
Main Methods:
- Utilizing a composite metamaterial slab.
- Integrating polarization rotation and selective absorption functionalities.
- Verifying the design through full-wave simulation and experimental microwave measurements.
Main Results:
- A one-way absorber with a thickness of one-sixth wavelength was designed and validated.
- Achieved over 83% absorption efficiency in one direction for a specific linearly polarized wave.
- Demonstrated over 83% transmission efficiency in the opposite direction for the same wave.
Conclusions:
- The proposed one-way absorber enables asymmetric transmission for linearly polarized waves.
- The composite metamaterial design shows potential for polarization control applications.
- This work highlights the versatility of metamaterials in creating multifunctional devices.
Related Concept Videos
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
Standing Waves in a Cavity
1.7K
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:
1.7K
Electromagnetic Wave Equation
2.7K
Maxwell's equations for electromagnetic fields are related to source charges, either static or moving. These fields act on a test charge, whose trajectory can thus be determined using suitable boundary conditions. The objective of electromagnetism is thus theoretically complete.
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations:...
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations:...
2.7K
Standing Electromagnetic Waves
2.5K
Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
2.5K
Plane Electromagnetic Waves II
4.3K
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.
4.3K
Electromagnetic Waves in Matter
4.3K
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,...
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,...
4.3K

