Related Experiment Video
Updated: Apr 26, 2026

11:57
Fabricating Metamaterials Using the Fiber Drawing Method
Published on: October 18, 2012
13.6K
Double-negative metamaterial from conducting spheres with a high-permittivity shell
Optics Letters
|August 1, 2014
Summary
We developed a novel three-dimensional metamaterial exhibiting double-negative behavior. This design uses metallic spheres with high-permittivity shells, enabling tunable negative refractive index properties for advanced electromagnetic applications.
Area of Science:
- Materials Science
- Electromagnetism
- Metamaterials
Background:
- Metamaterials offer unique electromagnetic properties not found in natural materials.
- Achieving double-negative behavior (simultaneously negative permittivity and permeability) is crucial for applications like negative refraction.
- Existing Mie resonance-based designs often rely on plasmonic behavior, limiting their operational frequencies and material choices.
Purpose of the Study:
- To propose a novel three-dimensional, isotropic metamaterial design.
- To achieve double-negative electromagnetic behavior using a different physical mechanism.
- To demonstrate the tunability of the metamaterial's properties.
Main Methods:
- Fabrication of a metamaterial composed of metallic spheres coated in a high-permittivity shell, dispersed within a host medium.
- Utilizing the metallic component as a near-perfect electric conductor, distinct from plasmonic approaches.
- Tuning the dimensions of the constituent particles to control the resonant frequencies.
Main Results:
- The proposed metamaterial exhibits double-negative behavior.
- The design relies on Mie resonances driven by the electric conductor nature of the metallic spheres.
- The operational frequency of the double-negative behavior is tunable by adjusting particle dimensions.
Conclusions:
- A novel, three-dimensional, isotropic metamaterial with double-negative properties has been successfully proposed.
- The design leverages near-perfect electric conductor behavior for Mie resonances, offering an alternative to plasmonic metamaterials.
- Tunable double-negative behavior is achievable across a wide range of frequencies by selecting appropriate high-conductivity and high-permittivity materials and adjusting particle dimensions.
Related Concept Videos
Electric Field of a Non Uniformly Charged Sphere
2.4K
Gauss's law states that the electric flux through any closed surface equals the net charge enclosed within the surface. This law is beneficial for determining the expressions for the electric field for a particular charge distribution if the electric flux is known.
Consider a non-uniformly charged sphere, for which the density of charge depends only on the distance from a point in space and not on the direction. Such a sphere has a spherically symmetrical charge distribution. Here, the electric...
Consider a non-uniformly charged sphere, for which the density of charge depends only on the distance from a point in space and not on the direction. Such a sphere has a spherically symmetrical charge distribution. Here, the electric...
2.4K
Electric Field of Parallel Conducting Plates
2.2K
Gauss' law relates the electric flux through a closed surface to the net charge enclosed by that surface. Gauss's law can be applied to find the electric field and the charge enclosed in a region depending on its charge distribution.
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric field, the...
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric field, the...
2.2K
Equipotential Surfaces and Conductors
5.1K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
5.1K
Gauss's Law in Dielectrics
5.8K
Consider a polar dielectric placed in an external field. In such a dielectric, opposite charges on adjacent dipoles neutralize each other, such that the net charge within the dielectric is zero. When a polar dielectric is inserted in between the capacitor plates, an electric field is generated due to the presence of net charges near the edge of the dielectric and the metal plates interface. Since the external electrical field merely aligns the dipoles, the dielectric as a whole is neutral. An...
5.8K
Theory of Metallic Conduction
2.0K
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
2.0K
Diamagnetic Shielding of Nuclei: Local Diamagnetic Current
1.3K
An applied magnetic field causes the electrons present in the molecule to circulate, setting up a local diamagnetic current within the molecule. The local diamagnetic current arising from circulating sigma-bonding electrons induces a magnetic field, Blocal that opposes the applied magnetic field, B0. The effective magnetic field experienced by these nuclei is given by the difference between the applied and local magnetic fields in a phenomenon called local diamagnetic shielding. Essentially,...
1.3K

