Related Experiment Video
Updated: May 1, 2026

12:19
Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
Published on: April 4, 2017
7.9K
Pulse compression in adiabatically tapered silicon photonic wires
Optics Express
|March 26, 2014
Summary
Engineered silicon photonic wire waveguides (Si-PhWWGs) achieve over 10x pulse compression at telecom and mid-IR wavelengths. This study analyzes optical field and free carrier dynamics for enhanced pulse manipulation.
Area of Science:
- Photonics
- Optical Engineering
- Materials Science
Background:
- Silicon photonic wire waveguides (Si-PhWWGs) are crucial for integrated optics.
- Pulse compression is vital for various optical applications, including spectroscopy and telecommunications.
- Understanding carrier dynamics is key to optimizing waveguide performance.
Purpose of the Study:
- To analyze pulse compression in Si-PhWWGs at telecom and mid-IR wavelengths.
- To investigate the coupled dynamics of optical fields and photogenerated free carriers.
- To explore the impact of waveguide geometry on pulse compression efficiency.
Main Methods:
- Theoretical and computational modeling of pulse propagation.
- Analysis of coupled optical field and free carrier dynamics.
- Simulation of adiabatically tapered Si-PhWWGs with varying physical and geometrical parameters.
Main Results:
- Achieved over 10x pulse compression in millimeter-long Si-PhWWGs.
- Demonstrated the influence of waveguide width engineering on linear and nonlinear optical properties.
- Identified inter-dependencies between pulse characteristics and compression efficiency.
Conclusions:
- Adiabatically tapered Si-PhWWGs offer a promising platform for significant pulse compression.
- Engineering waveguide geometry is an effective strategy to enhance pulse manipulation capabilities.
- The findings are relevant for both soliton and non-soliton pulse propagation regimes.
Related Concept Videos
Energy Stored In A Coaxial Cable
2.1K
A coaxial cable consists of a central copper conductor used for transmitting signals, followed by an insulator shield, a metallic braided mesh that prevents signal interference, and a plastic layer that encases the entire assembly.
In the simplest form, a coaxial cable can be represented by two long hollow concentric cylinders in which the current flows in opposite directions. The magnetic field inside and outside the coaxial cable is determined by using Ampère's law. The magnetic field...
In the simplest form, a coaxial cable can be represented by two long hollow concentric cylinders in which the current flows in opposite directions. The magnetic field inside and outside the coaxial cable is determined by using Ampère's law. The magnetic field...
2.1K
Propagation Speed of Electromagnetic Waves
3.1K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
3.1K
Lossless Lines
687
In electrical engineering, a lossless transmission line is characterized by a purely imaginary propagation constant and a resistive characteristic impedance. The ABCD parameters, which describe the relationship between the input and output voltages and currents, indicate an equivalent π circuit with an imaginary series impedance and a shunt admittance. This results in a transmission line that, when the product of the phase constant (beta) and the length of the line is less than pi,...
687
Joule-Thomson Effect
11.7K
The Joule-Thomson effect, also known as the Joule-Kelvin effect, describes the temperature change of a fluid when it is forced through a valve or porous plug while keeping it in a thermally insulated environment. This experiment is called a throttling process. This is an important effect widely used in refrigeration and the liquefaction of gases.
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
11.7K

