Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

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...
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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 semiconductor's...
Biasing of FET01:22

Biasing of FET

Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...
MOSFET: Enhancement Mode01:22

MOSFET: Enhancement Mode

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 current...
P-N junction01:11

P-N junction

A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Carrier-envelope phase control of ultrafast photocurrents in layered MoS<sub>2</sub>.

Optics express·2026
Same author

Redox-driven mineral and organic associations in Jezero Crater, Mars.

Nature·2025
Same author

PGMI assessment in mammography: AI software versus human readers.

Radiography (London, England : 1995)·2025
Same author

Technical feasibility of automated blur detection in digital mammography using convolutional neural network.

European radiology experimental·2024
Same author

Sb-saturated high-temperature growth of extended, self-catalyzed GaAsSb nanowires on silicon with high quality.

Nanotechnology·2023
Same author

Wafer-scale epitaxial modulation of quantum dot density.

Nature communications·2022

Related Experiment Video

Updated: May 18, 2026

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
15:47

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots

Published on: November 1, 2013

Electrical control of interdot electron tunneling in a double InGaAs quantum-dot nanostructure.

K Müller1, A Bechtold, C Ruppert

  • 1Walter Schottky Institut and Physik-Department, Technische Universität München, Am Coulombwall 4, 85748 Garching, Germany.

Physical Review Letters
|September 26, 2012
PubMed
Summary

We observed ultrafast electron tunneling between quantum dots using pump-probe spectroscopy. This tunneling, crucial for quantum computing, occurs via elastic and inelastic processes over a wide bandwidth.

More Related Videos

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

Related Experiment Videos

Last Updated: May 18, 2026

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
15:47

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots

Published on: November 1, 2013

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Spectroscopy

Background:

  • Electron tunneling is a fundamental quantum mechanical phenomenon.
  • Quantum dots are semiconductor nanocrystals with tunable electronic properties.
  • Understanding interdot electron transfer is key for developing quantum technologies.

Purpose of the Study:

  • To directly monitor electron tunneling between spatially separated quantum dots.
  • To investigate the role of Coulomb interactions and resonant tunneling processes.
  • To measure electron and hole tunneling times separately.

Main Methods:

  • Ultrafast pump-probe spectroscopy was employed.
  • The relative energy of orbital states in quantum dots was tuned.
  • Temporal evolution of pump-probe spectra was monitored.

Main Results:

  • Coulomb interactions influenced the photogenerated charge carriers.
  • Resonant tunneling was mediated by both elastic and inelastic processes.
  • Ultrafast interdot tunneling (<5 ps) occurred over a wide bandwidth (∼8 meV).

Conclusions:

  • Electron tunneling between quantum dots is directly observed and characterized.
  • The study reveals the mechanisms and timescales of interdot electron transfer.
  • Exciton-acoustic phonon coupling significantly influences the tunneling bandwidth.