Related Experiment Video
Updated: Dec 18, 2025

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
12.6K
Discontinuities in photonic waveguides: rigorous Maxwell-based 3D modeling with the finite element method
Summary
This study presents a general method for analyzing complex discontinuities in open waveguides using Maxwell
Area of Science:
- Computational Electromagnetics
- Waveguide Theory
- Plasmonics
Background:
- Studying discontinuities in open waveguides is crucial for designing advanced optical and sensing devices.
- Existing methods often struggle with complex, arbitrary shapes and rigorous vector analysis.
- Accurate modeling of plasmonic inclusions and periodic structures is challenging.
Purpose of the Study:
- To develop a general methodology for rigorous analysis of arbitrary discontinuities in open waveguides.
- To provide a framework for computing leaky modes and scattered fields.
- To validate the approach by comparing results with finite structures and demonstrating its applicability in infrared sensing.
Main Methods:
- Utilizing a full vector description based on Maxwell's equations within the finite element method (FEM).
- Computing leaky modes of the invariant structure and employing them as incident fields.
- Implementing a scattered field approach and projecting the scattered field onto the modes using bi-orthogonality.
Main Results:
- Successfully modeled general discontinuities, including arbitrary-shaped plasmonic inclusions.
- Computed complex propagation constants for periodically structured open waveguides.
- Demonstrated excellent agreement between the proposed method and finite structure simulations for an infrared sensing example.
Conclusions:
- The presented methodology offers a robust and general approach for analyzing complex waveguide discontinuities.
- The method accurately captures the behavior of open waveguides with arbitrary obstacles and periodic structuring.
- Open-source models are provided, facilitating reproducibility and further research in waveguide design and sensing applications.
Related Concept Videos
Differential Form of Maxwell's Equations
1.1K
James Clerk Maxwell (1831–1879) was one of the significant contributors to physics in the nineteenth century. He is probably best known for having combined existing knowledge of the laws of electricity and the laws of magnetism with his insights to form a complete overarching electromagnetic theory, represented by Maxwell's equations. The four basic laws of electricity and magnetism were discovered experimentally through the work of physicists such as Oersted, Coulomb, Gauss, and...
1.1K
Interference and Diffraction
51.2K
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.
51.2K
Electromagnetic Wave Equation
2.0K
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:...
2.0K
Electrostatic Boundary Conditions
847
Consider an external electric field propagating through a homogeneous medium. When the electric field crosses the surface boundary of the medium, it undergoes a discontinuity. The electric field can be resolved into normal and tangential components. The amount by which the field changes at any boundary is given by the difference between the field components above and below the surface boundary.
The surface integral of an electric field is given by Gauss's law in integral form and is related to...
The surface integral of an electric field is given by Gauss's law in integral form and is related to...
847
Limits with Oscillating Discontinuities
187
An oscillating discontinuity is a type of discontinuity in which a function’s values fluctuate infinitely often as the input approaches a particular point. Unlike jump discontinuities, where the function suddenly shifts between two values, or infinite discontinuities, where the function diverges without bound, an oscillating discontinuity arises from rapid back-and-forth variation. Because the function never stabilizes toward a single value, no finite limit exists at that point.One of the...
187
Symmetry in Maxwell's Equations
4.0K
Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
4.0K

