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Types Of Superconductors01:28

Types Of Superconductors

1.3K
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...
1.3K
Superconductor01:24

Superconductor

1.4K
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...
1.4K
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

1.5K
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,...
1.5K
Ferromagnetism01:31

Ferromagnetism

2.7K
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...
2.7K
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

404
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...
404
Paramagnetism01:30

Paramagnetism

2.8K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
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Related Experiment Video

Updated: Nov 3, 2025

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
04:51

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

Published on: July 8, 2021

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Tip-induced superconductivity.

Sandeep Howlader1, Goutam Sheet1

  • 1Department of Physical Sciences, Indian Institute of Science Education and Research Mohali, 81, Knowledge City, SAS Nagar, Manauli 140306, Punjab, India.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|June 4, 2021
PubMed
Summary
This summary is machine-generated.

Researchers explored a new method to achieve topological superconductivity by creating a tip-induced superconducting (TISC) phase in topological materials. This novel approach offers a promising avenue for realizing elusive quantum matter phases.

Keywords:
Andreev reflection spectroscopysuperconductivitytip-induced superconductivitytopological materials

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Area of Science:

  • Condensed Matter Physics
  • Quantum Materials Science
  • Superconductivity Research

Background:

  • Topological superconductivity is a sought-after quantum phase, often pursued by inducing superconductivity in topological insulators.
  • Previous methods like ion intercalation and pressure application on materials such as Bi2Se3 have not yielded conclusive evidence of topological superconductivity.
  • A significant gap exists in experimentally verifying superconductivity in confined, mesoscopic regions of topological materials.

Purpose of the Study:

  • To review a novel method for inducing superconductivity in non-superconducting topological materials via a mesoscopic interface.
  • To discuss the realization and characterization of the tip-induced superconducting (TISC) phase.
  • To highlight experimental signatures for detecting TISC in confined geometries where bulk methods fail.

Main Methods:

  • Creation of a mesoscopic interface between a normal metallic tip and a topological material.
  • Utilizing point-contact geometry to probe superconducting properties.
  • Investigating temperature and magnetic field dependent superconducting energy gap and critical current.

Main Results:

  • Successful realization of the tip-induced superconducting (TISC) phase in topological materials like Cd3As2.
  • Demonstration that TISC can emerge at a mesoscopic interface, distinct from bulk superconductivity.
  • Identification of specific experimental signatures suitable for detecting superconductivity in confined TISC regions.

Conclusions:

  • The TISC phase presents a viable pathway to achieving topological superconductivity in materials previously considered non-superconducting.
  • Mesoscopic point-contact spectroscopy offers crucial experimental signatures for TISC detection.
  • Further exploration of various topological material systems is warranted to realize the full potential of TISC.