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Related Concept Videos

Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
Ferromagnetism01:31

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...
Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

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...
Magnetism01:30

Magnetism

Magnets are commonly found in everyday objects, such as toys, hangers, elevators, doorbells, and computer devices. Experimentation on these magnets shows that all magnets have two poles: one is labeled north (N) and the other south (S). Magnetic poles repel if they are alike and attract if unlike. Moreover, both poles of a magnet attract unmagnetized pieces of iron.
An individual magnetic pole cannot be isolated. No matter how small, every piece of a magnet contains a north pole and a south...
Potential Due to a Magnetized Object01:24

Potential Due to a Magnetized Object

Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
Diamagnetism01:26

Diamagnetism

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.

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Updated: May 18, 2026

Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene
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Published on: July 3, 2015

Kondo screening and magnetism at interfaces.

A Euverte1, F Hébert, S Chiesa

  • 1INLN, Université de Nice-Sophia Antipolis, CNRS; 1361 route des Lucioles, 06560 Valbonne, France.

Physical Review Letters
|September 26, 2012
PubMed
Summary
This summary is machine-generated.

This study models metal-insulator interfaces, revealing how tuning hybridization impacts magnetic and transport properties. A Kondo insulating phase suppresses magnetism and conductivity, with magnetic order reappearing in outer layers as insulating layers increase.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Surface Science

Background:

  • Understanding magnetic order and transport at metal-insulator interfaces is crucial.
  • Heavy-fermion materials exhibit complex magnetic and electronic behaviors.

Purpose of the Study:

  • To model metal-insulator interfaces using a multilayer system.
  • To investigate the evolution of magnetic and transport properties with varying interface hybridization.

Main Methods:

  • Utilized a tight-binding Hamiltonian model for multilayer systems.
  • Tuned interface hybridization to observe changes in magnetic and metallic properties.

Main Results:

  • Observed competition between antiferromagnetism and Kondo singlet formation.
  • Identified a Kondo insulating phase at intermediate hybridization, suppressing magnetism and conductivity.
  • Magnetic order was restored in outer layers with increased insulating layers, but not at the interface.

Conclusions:

  • Interface hybridization significantly influences magnetic and transport properties.
  • Kondo physics effects persist in bulk layers near the interface.
  • No long-range magnetic order was detected in metallic layers.