Related Experiment Video
Updated: Jan 17, 2026

09:33
Demonstration of Equal-Intensity Beam Generation by Dielectric Metasurfaces
Published on: June 7, 2019
6.6K
Multichannel joint-polarization-frequency-modulation encrypted metasurface in secure THz communication.
Optics Express
|September 23, 2025
Summary
This study presents a novel metasurface for secure wireless communication. It uses amplitude-frequency modulation with graphene layers to encrypt data, enhancing security for terahertz applications.
Area of Science:
- Electromagnetic (EM) wave manipulation
- Metasurface technology
- Wireless communication security
Background:
- Wireless communication relies on EM signals for information transfer.
- Information encryption is vital to prevent counterfeiting and unauthorized access.
- Metasurfaces offer advanced control over EM wave properties.
Purpose of the Study:
- To introduce a metasurface for amplitude modulation at two distinct frequencies.
- To present an encrypted wireless communication protocol using a chaos algorithm.
- To enhance wireless communication security for terahertz (THz) applications.
Main Methods:
- Utilizing a metasurface with two distinct graphene layers for amplitude-frequency modulation.
- Implementing a chaos algorithm for data encryption.
- Simulating amplitude-frequency modulation for both x- and y-polarizations.
Main Results:
- Demonstrated simultaneous amplitude and frequency modulation for both linear polarizations.
- Achieved secure data transmission using graphene layers controlled by biasing conditions.
- Simulations confirmed successful encoding and transmission of image data.
Conclusions:
- The developed metasurface enables secure encrypted wireless communication.
- Simultaneous modulation of amplitude, frequency, and polarization enhances security and channel capacity.
- The protocol shows promise for THz communications, anti-counterfeiting, and data storage/transmission.
More Related Videos
Related Concept Videos
Propagation Speed of Electromagnetic Waves
4.6K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
4.6K
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
1.6K
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...
1.6K
Electromagnetic Waves
11.1K
James Clerk Maxwell formulated a single theory combining all the electric and magnetic effects scientists knew during that time, calling the phenomena his theory predicted “Electromagnetic waves”. He brought together all the work that had been done by brilliant physicists such as Oersted, Coulomb, Gauss, and Faraday and added his own insights to develop the overarching theory of electromagnetism. Maxwell’s equations, combined with the Lorentz force law, encompass all the laws...
11.1K
Electromagnetic Waves in Matter
3.9K
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,...
3.9K
IR Frequency Region: Fingerprint Region
1.9K
IR spectra are divided into two main regions: the diagnostic region and the fingerprint region. The diagnostic region of the spectrum lies above 1500 cm−1. The absorptions resulting from single-bond vibrations of the N–H, C–H, and O–H stretch at higher wavenumbers and appear on the left side of the spectrum. The stretching absorptions of the C≡C and C≡N occur between 2100–2300 cm−1. In contrast, those arising from stretching absorptions of the...
1.9K
IR Frequency Region: X–H Stretching
1.4K
In IR spectroscopy, signals produced by the X−H bonds (such as C−H, O−H, or N−H) can be observed in the frequency range of 2700–4000 cm–1. The C−H stretching vibration forms sharp bands in the region 2850–3000 cm–1. The presence of the O−H stretching vibration leads to the forming of an absorption band in the frequency range 3650–3200 cm−1. At the same time, N−H stretching can be confirmed by absorption bands in...
1.4K

