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Paramagnetism01:30

Paramagnetism

2.6K
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...
2.6K
Ferromagnetism01:31

Ferromagnetism

2.5K
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...
2.5K
Diamagnetism01:26

Diamagnetism

2.5K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.5K
Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

1.4K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.4K
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...
1.1K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

9.2K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
9.2K

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Related Experiment Video

Updated: Sep 10, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

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Magnetic impurities in a strongly coupled superconductor.

Samuel Ayodele Awelewa1, Maxim Dzero1

  • 1Department of Physics, Kent State University, Kent, OH 44242, United States of America.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|August 27, 2025
PubMed
Summary

Magnetic impurities influence metal superconductivity, especially with strong electron-phonon coupling. This study reveals unique superconducting behaviors, including re-entrant superconductivity and dual critical temperatures under specific magnetic exchange conditions.

Keywords:
Eliashberg theoryKondo effectsuperconductivity

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Mechanics

Background:

  • Superconductivity in metals is influenced by magnetic impurities.
  • Electron-phonon interaction is a key driver of superconductivity.
  • Understanding these interactions is crucial for developing novel superconducting materials.

Purpose of the Study:

  • To investigate the impact of magnetic impurities on superconducting properties.
  • To analyze the role of strong electron-phonon coupling in these phenomena.
  • To explore the formation of in-gap bound states and critical temperatures.

Main Methods:

  • Self-consistent solution of Nagaoka equations for the scattering matrix.
  • Application of Migdal-Eliashberg theory for superconductivity.
  • Computation of bound state energies, critical temperatures, and tunneling density of states.

Main Results:

  • Observed re-entrant superconductivity and a single pair of in-gap bound states for antiferromagnetic coupling.
  • Strong electron-phonon coupling reduces bound state decay length, enhancing localization.
  • Gapless superconductivity is achievable with lower impurity concentrations for antiferromagnetic exchange.
  • Ferromagnetic exchange coupling leads to a surprising two-critical-temperature superconducting transition.

Conclusions:

  • Magnetic impurities significantly alter superconducting properties, with effects dependent on coupling type and strength.
  • Strong electron-phonon coupling introduces unique localization effects for impurity-induced bound states.
  • The study highlights distinct superconducting behaviors under different magnetic exchange interactions, offering insights for material design.