Related Experiment Video
Updated: Feb 24, 2026

10:35
Using Microwave and Macroscopic Samples of Dielectric Solids to Study the Photonic Properties of Disordered Photonic Bandgap Materials
Published on: September 26, 2014
12.8K
Summary
A drifting optical potential on a discrete photonic lattice can become reflectionless when exceeding the light cone speed. This unique phenomenon for discrete light offers potential for novel optical devices.
Area of Science:
- Photonics
- Optical physics
- Condensed matter physics
Background:
- Light propagation in optical media is typically governed by wave equations.
- Continuous optical media exhibit predictable scattering phenomena.
- Discrete photonic lattices offer unique light-matter interaction properties.
Purpose of the Study:
- To investigate the behavior of optical potentials in discrete photonic lattices.
- To explore the conditions under which an optical potential becomes reflectionless.
- To examine the implications of discrete translational symmetry on light scattering.
Main Methods:
- Theoretical analysis of optical potentials on discrete photonic lattices.
- Investigating the effect of transverse drift speed exceeding the light cone speed.
- Considering non-Hermitian optical potentials of the Kramers-Kronig type.
Main Results:
- An arbitrarily shaped optical potential becomes reflectionless when drifting faster than the lattice band's light cone speed.
- This reflectionless property is unique to discrete photonic systems and lacks counterparts in continuous media.
- A drifting non-Hermitian Kramers-Kronig potential acts as an invisible potential, allowing undistorted beam propagation.
Conclusions:
- Discrete translational symmetry in photonic lattices enables novel optical phenomena like reflectionless potentials.
- The concept of an 'invisible potential' is demonstrated for discrete optical beams.
- Findings suggest new possibilities for controlling light propagation in engineered photonic structures.
Related Concept Videos
Bewley Lattice Diagram
1.5K
The Bewley lattice diagram, developed by L. V. Bewley, effectively organizes the reflections occurring during transmission-line transients. It visually represents how voltage waves propagate and reflect within a transmission line, making it easier to understand the complex interactions that occur.
1.5K
Interference and Diffraction
52.8K
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.
52.8K
Poisson's And Laplace's Equation
4.4K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
4.4K
The de Broglie Wavelength
33.9K
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...
33.9K
The Wave Nature of Light
62.4K
The nature of light has been a subject of inquiry since antiquity. In the seventeenth century, Isaac Newton performed experiments with lenses and prisms and was able to demonstrate that white light consists of the individual colors of the rainbow combined together. Newton explained his optics findings in terms of a "corpuscular" view of light, in which light was composed of streams of extremely tiny particles traveling at high speeds according to Newton's laws of motion.
62.4K
Potential Due to a Polarized Object
837
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
837

