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Related Concept Videos

Potential Due to a Magnetized Object01:24

Potential Due to a Magnetized Object

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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...
248
Paramagnetism01:30

Paramagnetism

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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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Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

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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...
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Diamagnetism01:26

Diamagnetism

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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....
2.4K
Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

838
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...
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Ferromagnetism01:31

Ferromagnetism

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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...
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Bending altermagnetic films creates a novel curvature-induced magnetization. This effect allows for imaging magnetic domain structures in compensated materials and depends on bending direction and altermagnetic symmetry.

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Area of Science:

  • Condensed Matter Physics
  • Magnetism
  • Materials Science

Background:

  • Altermagnetism in magnetically ordered materials leads to unique physical effects.
  • Curvilinear magnetism in low-dimensional systems presents novel phenomena.

Purpose of the Study:

  • To investigate the novel physical effect arising from the combination of altermagnetism and curvilinear magnetism.
  • To explore curvature-induced magnetization in bent altermagnetic films.
  • To establish a method for imaging domain structures in magnetically compensated materials.

Main Methods:

  • Theoretical analysis of a thin d-wave altermagnet film bent in a stretching-free manner.
  • Analytical calculations of magnetization, magnetic moment, and toroidal moment.
  • Numerical spin-lattice simulations to validate analytical predictions.

Main Results:

  • Gradients in film curvature induce local, tangential magnetization.
  • Magnetization amplitude is dependent on altermagnetic symmetry and bending direction.
  • Periodically bent films and rolled-up nanotubes exhibit unique magnetic moments proportional to bending parameters.

Conclusions:

  • Curvature-induced magnetization is a novel effect in bent altermagnetic films.
  • This phenomenon offers a new pathway for visualizing magnetic domain structures.
  • The study provides a theoretical framework and simulation-based validation for these effects.