Related Experiment Video
Updated: Nov 1, 2025

15:47
Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
Published on: November 1, 2013
16.5K
Optimized plasmonic reversible logic gate for low loss communication
Applied Optics
|June 18, 2021
Summary
This study presents a novel plasmonic optical waveguide design for a Feynman logic gate, significantly reducing power consumption and information loss for reversible computing applications.
Area of Science:
- Optoelectronics
- Nanophotonics
- Plasmonics
Background:
- Reversible computing requires logic gates to minimize information loss and power consumption.
- Plasmonic optical waveguides enable controlled fabrication of nanostructures for advanced optical devices.
Purpose of the Study:
- To design and simulate a Feynman logic gate using a metal-insulator-metal optical waveguide.
- To evaluate the performance of the proposed Feynman logic gate in terms of footprint, extinction ratio, and insertion loss.
Main Methods:
- Simulation of the Feynman logic gate using a cascading metal-insulator-metal optical waveguide based on Mach-Zehnder interferometers.
- Utilizing the finite difference time domain (FDTD) method for numerical simulation.
- Verification of simulation results through mathematical computation in MATLAB.
Main Results:
- The proposed Feynman logic gate achieves a footprint of 62 µm × 9 µm.
- The device exhibits an extinction ratio of 10.57 dB.
- Insertion losses are measured at -0.969 dB and -1.191 dB, outperforming existing electro-optic designs.
Conclusions:
- The developed plasmonic optical waveguide Feynman logic gate offers superior performance compared to electro-optic alternatives.
- This design is a promising advancement for low-power, high-efficiency reversible computing systems.
Related Concept Videos
MOSFET: Enhancement Mode
553
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
553
Biasing of Metal-Semiconductor Junctions
403
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...
403
Metal-Semiconductor Junctions
603
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...
603
MOSFET: Depletion Mode
558
Depletion-mode MOSFETs represent a unique subset of MOSFET technology, functioning fundamentally differently from their enhancement-mode counterparts. Unlike enhancement MOSFETs, which require a positive gate-source voltage (Vgs) to turn on, depletion-mode MOSFETs are inherently conductive and "normally on" devices.
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity...
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity...
558

