Related Experiment Video
Updated: Feb 12, 2026

Preparation of Silicon Nanowire Field-effect Transistor for Chemical and Biosensing Applications
Published on: April 21, 2016
Field-tunable charge confinement in III-V layered nanowire-array superlattices
Reyna Méndez-Camacho1, Esteban Cruz-Hernández2, Máximo López-López1
1Physics Department, Centro de Investigación y de Estudios Avanzados del IPN, 07360, Mexico City, Mexico.
None:
We present a theoretical framework for electric-field control of charge confinement and interwire tunneling in GaAs/AlGaAs layered nanowire-array superlattices. Using a two-electron effective mass model that incorporates screened Coulomb interaction and experimentally realistic confinement geometries, we investigate how transverse electric fields and structural design parameters enable tunable redistribution of charge carriers across vertically stacked quantum wires. Our results reveal a crossover from delocalized miniband-like states to strongly localized charge layers, driven by the interplay between quantum confinement, interwire coupling, and electrostatic potential gradients under dielectric screening. We further outline a feasible implementation based on the self-assembly of GaAs nanowire arrays grown on high-index substrates via molecular beam epitaxy, providing a lithography-free route toward scalable coupled-wire architectures. The demonstrated field-tunable confinement opens new possibilities for programmable optoelectronic platforms, enabling charge-selective transport, sensing, and reconfigurable nanophotonic architectures, and highlights new pathways for the integration of III-V nanostructures into quantum and optoelectronic device technologies.
More Related Videos
Related Concept Videos
Electric Field of a Continuous Line Charge
In calculations of electric fields, symmetry is of great use. For example, while calculating electric fields of continuous charge distributions.
Consider a line element with a...
Electric Field of Two Equal and Opposite Charges
A separation of the positive and negative charges can lead to a weak, remnant effect of the positive and negative charges. The expectation is that the more the distance between the positive and...
Electric Field of a Charged Disk
The system's symmetry is in the cylindrical directions across the plane of the charge. As a result, the electric fields created by various surface charge elements nullify each other in the direction parallel to the surface. Thereby, the resulting electric field is perpendicular to the plane. Since the disk is...
Magnetic Field due to Moving Charges
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Motion Of A Charged Particle In A Magnetic Field
Electric Field of a Non Uniformly Charged Sphere
Consider a non-uniformly charged sphere, for which the density of charge depends only on the distance from a point in space and not on the direction. Such a sphere has a spherically symmetrical charge distribution. Here, the electric...

