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Types Of Superconductors01:28

Types Of Superconductors

1.1K
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...
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Superconductor01:24

Superconductor

1.2K
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...
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Types of Semiconductors01:20

Types of Semiconductors

843
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
843
Fermi Level01:18

Fermi Level

730
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
730
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

429
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...
429
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

1.4K
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,...
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Related Experiment Video

Updated: Aug 17, 2025

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

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Interface Superconductivity in a Dirac Semimetal NiTe2.

Varnava D Esin1, Oleg O Shvetsov1, Anna V Timonina1

  • 1Institute of Solid State Physics of the Russian Academy of Sciences, Moscow District, 2 Academician Ossipyan Str., 142432 Chernogolovka, Russia.

Nanomaterials (Basel, Switzerland)
|December 11, 2022
PubMed
Summary
This summary is machine-generated.

Researchers observed interfacial superconductivity in a Nickel Telluride (NiTe2) Dirac semimetal junction. This phenomenon, driven by flat bands, supports Josephson current and a Josephson diode effect.

Keywords:
Dirac materialssuperconductivitytopological semimetals

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Phenomena

Background:

  • Dirac semimetals exhibit unique electronic properties with potential for novel quantum effects.
  • Interfacial phenomena can lead to emergent properties not present in bulk materials.
  • Superconductivity and topological states are key areas of research in condensed matter physics.

Purpose of the Study:

  • To experimentally investigate charge transport at a NiTe2 Dirac semimetal and gold interface.
  • To explore the possibility of interfacial superconductivity induced by flat-band formation.
  • To demonstrate and analyze the Josephson diode effect in this system.

Main Methods:

  • Experimental measurement of charge transport (dV/dI(V)) at milli-Kelvin temperatures.
  • Utilizing a single planar junction between NiTe2 and a normal gold lead.
  • Applying temperature and magnetic field variations to study the observed phenomena.
  • Investigating Josephson current through topological surface states.

Main Results:

  • Observed non-Ohmic dV/dI(V) behavior indicative of Andreev reflection at the interface.
  • Demonstrated suppression of the effect with increasing temperature and magnetic field, supporting superconductivity.
  • Confirmed interfacial superconductivity attributed to flat-band formation at the Au-NiTe2 interface.
  • Showcased a pronounced Josephson diode effect arising from topological surface states.

Conclusions:

  • The NiTe2-Au interface exhibits superconductivity, distinct from the bulk NiTe2 properties.
  • Flat-band formation at the interface is the likely mechanism driving the observed superconductivity.
  • The topological surface states of NiTe2 support Josephson current and enable a Josephson diode effect.
  • This study highlights the potential of Dirac semimetals for novel superconducting and spintronic devices.