Related Experiment Video
Updated: May 28, 2026

11:33
All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
Published on: January 19, 2018
Evidence of surface charge effects in T-branch nanojunctions using microsecond-pulse testing.
I Iñiguez-de-la-Torre1, J Mateos, Y Roelens
1Departamento de Física Aplicada, Universidad de Salamanca, Salamanca, Spain.
Nanotechnology
|October 13, 2011
Summary
This study reveals how surface charge affects nanostructure electrical properties using ultrafast electrical pulses. The T-branch nanojunction
Area of Science:
- Nanotechnology
- Surface Science
- Electrical Engineering
Background:
- Surface charge effects are critical for advanced electronic devices.
- Understanding nanostructure electrical properties is essential for future technologies.
Purpose of the Study:
- To investigate the room-temperature time response of a T-branch nanojunction.
- To identify the signature of surface states using ultrafast electrical pulse characterization.
- To elucidate the influence of surface charge on electrical properties.
Main Methods:
- Employed an ultrafast electrical pulse characterization technique.
- Applied varying pulse widths (500 ns to 100 µs) to a T-branch nanojunction.
- Measured and compared stem voltage with DC results for different pulse widths.
Main Results:
- The nanojunction's time response was characterized at room temperature.
- The stem voltage output demonstrated dependence on pulse width.
- Results indicated a relationship between pulse width and the characteristic charging time of interface states.
Conclusions:
- Surface states signatures were identified in the T-branch nanojunction's response.
- The nonlinear response of T-branch junctions becomes more pronounced with longer pulses, exceeding a characteristic time.
- This research provides key insights into surface charge effects in nanostructures.
Related Concept Videos
Biasing of P-N Junction
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...
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...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
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...
Junction Potentials in Galvanic Cells
The Nernst equation, derived under the assumption of thermodynamic equilibrium, calculates the electromotive force (emf) as the sum of potential differences at phase boundaries in a reversible cell without a liquid junction. However, in irreversible cells such as the Daniell cell, an additional potential difference named the liquid-junction potential (EJ) arises across the interface of two electrolyte solutions due to different ion diffusion rates. This EJ represents the potential difference...
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...
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...

