Related Experiment Video
Updated: May 18, 2026

07:14
Iron Nanowire Fabrication by Nano-Porous Anodized Aluminum and its Characterization
Published on: October 6, 2019
Superconductor-insulator transition in long MoGe nanowires
Hyunjeong Kim1, Shirin Jamali, A Rogachev
1Department of Physics and Astronomy, University of Utah, Salt Lake City, Utah 84112, USA.
Physical Review Letters
|October 4, 2012
Summary
Researchers studied narrow superconducting wires to understand the superconductor-insulator transition (SIT). They found the transition depends on wire dimensions and magnetic fields, challenging current theories.
Area of Science:
- Condensed Matter Physics
- Materials Science
Background:
- Superconducting properties are influenced by physical processes at various length scales.
- Understanding the critical regime in one-dimensional superconductors is crucial for device applications.
Purpose of the Study:
- To identify the dominant physical process in the critical regime of one-dimensional superconducting wires.
- To investigate the factors controlling the superconductor-insulator transition (SIT) in narrow MoGe wires.
Main Methods:
- Fabrication of very narrow (9-20 nm) MoGe wires using electron-beam lithography.
- Systematic study of transport properties across a wide range of wire lengths (1-25 μm).
- Application of external magnetic fields to induce transitions.
Main Results:
- Observed a superconductor-insulator transition (SIT) controlled by the wire's cross-sectional area and potentially its width-to-thickness ratio.
- Found that the mean-field critical temperature decreases exponentially with the inverse of the wire's cross section.
- Demonstrated that a similar SIT can be induced by an external magnetic field.
- Identified some long superconducting MoGe nanowires exhibiting localized superconductivity where localization length is smaller than wire length.
Conclusions:
- The observed SIT in narrow MoGe wires is not explained by current theories.
- Wire dimensions and magnetic fields are key parameters controlling the SIT.
- Localization effects play a significant role in the behavior of long superconducting nanowires.
More Related Videos
Related Concept Videos
Types Of Superconductors
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
Superconductor
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
Theory of Metallic Conduction
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
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...
Magnetic Field Due To A Thin Straight Wire
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
Ferromagnetism
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...

