Related Experiment Video
Updated: Mar 12, 2026

07:28
Terahertz Microfluidic Sensing Using a Parallel-plate Waveguide Sensor
Published on: August 30, 2012
11.2K
Thin-wall tubes for coupling terahertz waves to metal wires
Applied Optics
|November 19, 2016
Summary
A novel thin-wall tube efficiently couples terahertz (THz) waves to metal wires, achieving 94% efficiency. This method optimizes field matching for enhanced plasmon polariton guiding.
Area of Science:
- Optics and Photonics
- Materials Science
- Electromagnetism
Background:
- Metal wires are key for guiding terahertz (THz) surface plasmon polaritons.
- Efficiently coupling THz waves to these waveguides remains a challenge.
Purpose of the Study:
- To propose a thin-wall tube structure for ultrahigh-efficiency THz wave coupling to metal wires.
- To investigate the factors influencing coupling efficiency.
Main Methods:
- Mode-overlap calculations were performed to determine coupling efficiency.
- Analysis focused on field distributions, polarization directions, and wave vectors.
- Simulations covered THz frequencies from 0.2-3 THz with a 0.5 mm wire radius.
Main Results:
- The proposed thin-wall tube achieved coupling efficiencies between 84% and 94% across the 0.2-3 THz range.
- A maximum efficiency of 94% was observed at 0.5 THz.
- This significantly surpasses efficiencies reported for previous coupling methods.
Conclusions:
- The thin-wall tube offers a highly efficient method for THz wave coupling to metal wires.
- Optimal coupling occurs when the outer tube radius matches the wire radius and propagation constants are equal.
Related Concept Videos
Magnetic Field Due To A Thin Straight Wire
6.4K
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
6.4K
Magnetic Field Due to Two Straight Wires
5.1K
Consider two parallel straight wires carrying a current of 10 A and 20 A in the same direction and separated by a distance of 20 cm. Calculate the magnetic field at a point "P2", midway between the wires. Also, evaluate the magnetic field when the direction of the current is reversed in the second wire.
5.1K
Metal-Semiconductor Junctions
1.2K
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
1.2K
Biasing of Metal-Semiconductor Junctions
743
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
743
Standing Waves in a Cavity
1.6K
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:
1.6K

