Related Experiment Video
Updated: Oct 14, 2025

15:06
Measurement of Scattering Nonlinearities from a Single Plasmonic Nanoparticle
Published on: January 3, 2016
13.0K
Modal approximation for plasmonic resonators in the time domain: the scalar case.
Lorenzo Baldassari1, Pierre Millien2, Alice L Vanel1
1Department of Mathematics, ETH Zürich, Rämistrasse 101, 8092 Zurich, Switzerland.
Summary
We developed a new method to approximate electromagnetic fields scattered by metallic nanoparticles. This approach accurately predicts the field behavior in both frequency and time domains using modal analysis.
Area of Science:
- Electromagnetism and Optics
- Computational Physics
Background:
- Understanding electromagnetic scattering from nanoparticles is crucial for optical applications.
- Dispersive material properties and resonant regimes present significant theoretical challenges.
Purpose of the Study:
- To develop a modal approximation for electromagnetic fields scattered by metallic nanoparticles.
- To analyze the behavior of these fields in low-frequency and resonant regimes.
- To validate the approximation through numerical simulations.
Main Methods:
- Defining non-Hermitian modes as perturbations of electro-static modes.
- Obtaining a frequency-domain modal approximation of the scattered field.
- Analyzing the eigenvalues of a singular boundary integral operator.
- Presenting two-dimensional numerical simulations.
Main Results:
- The poles of the modal expansion correspond to eigenvalues in the lower-half complex plane.
- The modal representation provides a highly accurate approximation of the scattered field.
- Numerical simulations confirm the validity of the modal approach.
Conclusions:
- The developed modal representation accurately describes electromagnetic scattering from dispersive metallic nanoparticles.
- This method offers a powerful tool for analyzing nanoparticle optics in resonant regimes.
- The findings have implications for designing optical devices and metamaterials.
Related Concept Videos
Standing Waves in a Cavity
1.1K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.1K
Linear Approximation in Frequency Domain
166
Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
166
Parallel Resonance
294
The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
294
Linear Approximation in Time Domain
140
Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
140

