Related Experiment Video
Updated: Dec 30, 2025

11:13
Analysis of Contact Interfaces for Single GaN Nanowire Devices
Published on: November 15, 2013
9.7K
Controllable p-n junctions in three-dimensional Dirac semimetal Cd3As2 nanowires.
Janice Ruth Bayogan1,2, Kidong Park3, Zhuo Bin Siu4
1Department of Emerging Materials Science, DGIST, Daegu 42988, Republic of Korea.
Nanotechnology
|January 22, 2020
Summary
We demonstrate tunable p-n junctions in cadmium arsenide (Cd3As2) nanowires, enabling quantum dot behavior and electron optics for novel quantum devices.
Area of Science:
- Condensed matter physics
- Materials science
- Nanotechnology
Background:
- Three-dimensional Dirac semimetals (DSMs) possess unique electronic properties.
- Cd3As2 is a prominent DSM material with potential for electronic applications.
- Controlling charge carriers in semimetals is crucial for device fabrication.
Purpose of the Study:
- To demonstrate a controllable p-n junction in a Cd3As2 nanowire.
- To investigate the electronic transport properties under gate voltage and magnetic fields.
- To explore the potential for quantum devices based on DSM nanowires.
Main Methods:
- Fabrication of a Cd3As2 nanowire device with two recessed bottom gates.
- Electrical transport measurements under varying gate voltages and perpendicular magnetic fields.
- Analysis of conductance regimes and quantum phenomena.
Main Results:
- Achieved four distinct conductance regimes (unipolar and bipolar) by tuning gate voltages, indicating controllable p-n junction formation.
- Observed a drastic decrease in conductance in p-n junction regimes under perpendicular magnetic fields.
- Demonstrated quantum dot behavior in p-n junction regimes and conductance plateaus in the n-n regime at high magnetic fields.
Conclusions:
- Ambipolar tunability of DSM nanowires is feasible.
- Cd3As2 nanowires can be utilized to create quantum devices.
- The findings pave the way for novel quantum dots and electron optics applications.
Related Concept Videos
P-N junction
1.0K
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...
1.0K
Biasing of Metal-Semiconductor Junctions
495
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...
495
Biasing of P-N Junction
1.6K
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
1.6K
Metal-Semiconductor Junctions
818
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...
818

