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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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An applied magnetic field causes the electrons present in the molecule to circulate, setting up a local diamagnetic current within the molecule. The local diamagnetic current arising from circulating sigma-bonding electrons induces a magnetic field, Blocal that opposes the applied magnetic field, B0. The effective magnetic field experienced by these nuclei is given by the difference between the applied and local magnetic fields in a phenomenon called local diamagnetic shielding. Essentially,...
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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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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.
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An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
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Atomic Nuclei: Nuclear Magnetic Moment00:59

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All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
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Competitive Size Effects in Antiferromagnetic|Ferrimagnetic Core|Shell Nanoparticles for Large Exchange Bias.

Alberto López-Ortega1,2, Beatrice Muzzi3,4, Cesar de Julián Fernández5

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The size of antiferromagnetic (AFM) and ferrimagnetic (FiM) components in core-shell nanoparticles significantly impacts their magnetic properties and exchange-bias effects. Smaller particle dimensions can lead to unique magnetic behaviors, influencing potential applications in spintronics and rare-earth-free magnets.

Keywords:
antiferromagnetblocking temperaturecore|shellexchange biasnanoparticles

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Nanotechnology

Background:

  • Exchange-coupled core-shell (CS) nanoparticles combine antiferromagnetic (AFM) and ferrimagnetic (FiM) materials.
  • The interplay between core and shell dimensions is crucial for tuning magnetic properties.
  • Understanding size-dependent magnetic behavior is key for advanced nanomaterials.

Purpose of the Study:

  • To investigate the role of core and shell dimensions in AFM/FiM core-shell nanoparticles.
  • To elucidate the influence of particle size on exchange-bias phenomena.
  • To explore the potential of these nanomaterials in technological applications.

Main Methods:

  • Synthesis of core-shell nanoparticles with varying core diameters (2, 5, 16 nm) and fixed shell thickness (~2 nm).
  • Composition: Antiferromagnetic Co$_{0.3}$Fe$_{0.7}$O core and ferrimagnetic Co$_{0.6}$Fe$_{2.4}$O$_{4}$ shell.
  • Magnetic property characterization focusing on exchange-bias effects and temperature-dependent transitions.

Main Results:

  • Strong magnetic coupling observed between core and shell in all samples.
  • Size significantly influences magnetic properties: larger particles exhibit classic exchange-bias (TC > TN).
  • Smaller particles show reduced blocking temperatures for the FiM shell and potential blocking transitions in the AFM core, indicating size-dependent magnetic fluctuations and ordering.

Conclusions:

  • The dimensions of both AFM and FiM components critically determine the magnetic properties of core-shell nanoparticles.
  • Size reduction leads to altered exchange-bias mechanisms, shifting from AFM core ordering to FiM shell thermal fluctuations.
  • Findings are relevant for designing nanodevices utilizing exchange-bias, with potential applications in rare-earth-free magnets, spintronics, and magnetic refrigeration.