Related Experiment Video
Updated: May 1, 2026

13:44
Simulation, Fabrication and Characterization of THz Metamaterial Absorbers
Published on: December 27, 2012
15.0K
Near-perfect absorption in epsilon-near-zero structures with hyperbolic dispersion
Optics Express
|March 26, 2014
Summary
Hyperbolic metamaterials exhibit enhanced electromagnetic energy absorption compared to conventional materials, especially when their thickness is subwavelength. Near-perfect absorption is achieved when the normal permittivity component approaches zero.
Area of Science:
- Physics
- Materials Science
- Electromagnetism
Background:
- Metamaterials offer unique electromagnetic properties.
- Hyperbolic metamaterials feature anisotropic permittivity (εx and εz have opposite signs).
Purpose of the Study:
- To investigate electromagnetic wave absorption in hyperbolic metamaterials.
- To explore the effect of subwavelength thickness on absorption.
- To identify conditions for enhanced absorption.
Main Methods:
- Theoretical analysis of polarized electromagnetic wave interaction.
- Modeling hyperbolic metamaterial structures with specific permittivity properties (εx * εz < 0).
Main Results:
- Hyperbolic metamaterials show significantly higher electromagnetic energy absorption than conventional materials for subwavelength thicknesses.
- Near-perfect absorption is observed for wavelengths where the real part of the normal permittivity component (ℜ(εz)) is approximately zero.
- This absorption band is robust across a range of frequencies and structure thicknesses.
Conclusions:
- Subwavelength hyperbolic metamaterials are highly efficient absorbers of electromagnetic energy.
- Tuning metamaterial properties to achieve ℜ(εz) ≈ 0 is a promising strategy for broadband, near-perfect absorption applications.
More Related Videos
Related Concept Videos
NMR Spectrometers: Resolution and Error Correction
993
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
993
¹H NMR: Interpreting Distorted and Overlapping Signals
1.3K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.3K
Geometry of Hyperbolas
693
A hyperbola consists of all points where the absolute difference of distances to two fixed points, called foci, remains constant. The standard equation isEach branch extends infinitely and approaches two asymptotes, which guide the curve’s behavior. The parameters a and b define key features: a measures the distance from the center to each vertex along the transverse axis, while b influences the slopes of the asymptotes. The asymptotes have equationsA rectangle centered at the origin with...
693
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
1.3K
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
1.3K
The de Broglie Wavelength
25.7K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.7K
UV–Vis Spectrum
3.1K
When light passes through a substance, a portion of the light is absorbed while the remaining light is reflected or transmitted. If the molecule absorbs light between the wavelengths of 180–400 nm range, the UV spectrum is obtained, and if it absorbs light in the 400–780 nm wavelength range, the visible spectrum is obtained.
The UV–Vis spectrum of a molecule is the plot of its absorbance versus wavelength. The plot is drawn by taking molar...
The UV–Vis spectrum of a molecule is the plot of its absorbance versus wavelength. The plot is drawn by taking molar...
3.1K

