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Related Concept Videos

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...
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...
Bipolar Junction Transistor01:22

Bipolar Junction Transistor

Bipolar Junction Transistors (BJTs) are essential elements in electronic circuits, playing a crucial role in the functionality of amplifiers, memories, and microprocessors. These transistors can be designed as NPN or PNP based on their doping patterns. They consist of three layers: the emitter, base, and collector. The configuration of these layers and their respective doping levels—with N-type or P-type impurities—define the transistor's type and its operational characteristics.
The structure...
Semiconductors01:22

Semiconductors

There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Field Effect Transistor01:29

Field Effect Transistor

Field-effect transistors (FETs) are integral to electronic circuits and distinguished by their three-terminal setup: the gate, drain, and source. These transistors operate as unipolar devices, which utilize either electrons or holes as charge carriers, in contrast to bipolar transistors, which use both types of carriers. The primary function of the FET is to modulate the flow of these carriers from the source to the drain through a channel. The voltage difference between the gate and source...
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...

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Related Experiment Video

Updated: Jun 16, 2026

Flow-assisted Dielectrophoresis: A Low Cost Method for the Fabrication of High Performance Solution-processable Nanowire Devices
09:14

Flow-assisted Dielectrophoresis: A Low Cost Method for the Fabrication of High Performance Solution-processable Nanowire Devices

Published on: December 7, 2017

Nanowire transistors without junctions.

Jean-Pierre Colinge1, Chi-Woo Lee, Aryan Afzalian

  • 1Tyndall National Institute, University College Cork, Lee Maltings, Cork, Ireland. jean-pierre.colinge@tyndall.ie

Nature Nanotechnology
|February 23, 2010
PubMed
Summary
This summary is machine-generated.

Researchers developed new junctionless transistors using silicon nanowires. These novel devices overcome fabrication challenges in modern electronics, offering improved performance and reduced leakage currents.

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Area of Science:

  • Semiconductor Physics
  • Materials Science
  • Nanotechnology

Background:

  • Existing transistors rely on semiconductor junctions, requiring high doping concentration gradients.
  • Fabricating junctions below 10 nm presents significant challenges due to diffusion laws and atomic distribution.
  • These limitations hinder the advancement of modern semiconductor devices.

Purpose of the Study:

  • To propose and demonstrate a novel transistor design eliminating the need for junctions and doping gradients.
  • To explore the fabrication and functionality of junctionless transistors using silicon nanowires.
  • To evaluate the performance characteristics of these new devices compared to classical transistors.

Main Methods:

  • Fabrication of transistors using silicon nanowires.
  • Characterization of device functionality and performance metrics.
  • Analysis of subthreshold slope, leakage currents, and carrier mobility.

Main Results:

  • Demonstrated full CMOS functionality in junctionless transistors.
  • Achieved near-ideal subthreshold slope and extremely low leakage currents.
  • Observed less degradation of mobility with gate voltage and temperature compared to classical transistors.

Conclusions:

  • Junctionless transistors offer a viable alternative to traditional designs, overcoming critical fabrication hurdles.
  • Silicon nanowire-based junctionless transistors exhibit superior electrical characteristics.
  • This technology holds promise for future high-performance, low-power electronic devices.