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Related Concept Videos

The Hall Effect01:30

The Hall Effect

Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
Paramagnetism01:30

Paramagnetism

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...
Magnetic Fields01:27

Magnetic Fields

A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
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...
Motional Emf01:22

Motional Emf

Magnetic flux depends on three factors: the strength of the magnetic field, the area through which the field lines pass, and the field's orientation with respect to the surface area. If any of these quantities vary, a corresponding variation in magnetic flux occurs. If the area through which the magnetic field lines are passing changes, then the magnetic flux also changes. This change in the area can be of two types: the flux through the rectangular loop increases as it moves into the magnetic...
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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Related Experiment Video

Updated: May 26, 2026

Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene
08:25

Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene

Published on: July 3, 2015

Energy magnetization and the thermal Hall effect.

Tao Qin1, Qian Niu, Junren Shi

  • 1Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.

Physical Review Letters
|December 21, 2011
PubMed
Summary

This study introduces general formulas for magnetizations, correcting thermal transport coefficients in magnetic systems. It resolves unphysical divergences in calculations, ensuring accurate thermal conductivity for systems like the anomalous Hall effect.

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Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
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Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials

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Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene
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Chemical Vapor Deposition of an Organic Magnet, Vanadium Tetracyanoethylene

Published on: July 3, 2015

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
10:36

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials

Published on: January 21, 2016

Area of Science:

  • Condensed Matter Physics
  • Thermodynamics
  • Electromagnetism

Background:

  • Evaluating thermal transport coefficients in magnetic systems is complex.
  • Direct application of the Kubo formula can lead to unphysical divergences.
  • Magnetization effects on thermal transport require a systematic theoretical framework.

Purpose of the Study:

  • To derive general formulas for magnetizations, including electromagnetic and gravitomagnetic energy magnetization.
  • To demonstrate magnetization corrections to thermal transport coefficients.
  • To provide a systematic approach for evaluating thermal transport coefficients in magnetic systems.

Main Methods:

  • Derivation of general formulas for magnetizations.
  • Explicit demonstration of magnetization corrections to thermal transport coefficients.
  • Application of the derived theory to noninteracting anomalous Hall systems.

Main Results:

  • General formulas for electromagnetic and gravitomagnetic energy magnetization were obtained.
  • Magnetization corrections to thermal transport coefficients were explicitly shown.
  • The corrected thermal Hall conductivity for a noninteracting anomalous Hall system was found to obey the Wiedemann-Franz law.

Conclusions:

  • The developed theory offers a systematic method for calculating thermal transport coefficients in magnetic systems.
  • The approach eliminates unphysical divergences encountered with direct Kubo formula application.
  • The findings validate the Wiedemann-Franz law for corrected thermal Hall conductivity in specific systems.