The magnetic anisotropy is the difference between the energy required to magnetize the element in contraction single variant state and in elongation single variant state.
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Because of the nanoparticle s magnetic anisotropy, the magnetic moment has usually only two stable orientations antiparallel to each other, separated by an energy barrier.
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Magnetic anisotropy, that is the existence of an easy direction along which the moments align spontaneously in the crystal, corresponds however to " massive " magnons.
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It is a " soft " magnetic material; it has low magnetic anisotropy and magnetostriction, giving it a low coercivity so that it saturates at low magnetic fields.
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For remanence to be possible there must be a strong enough magnetic anisotropy to keep the magnetization near a stable state; otherwise, thermal fluctuations make the magnetic moment wander randomly.
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First, the crystal lattice of most magnetic materials has magnetic anisotropy, which means it has an " easy " direction of magnetization, parallel to one of the crystal axes.
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The magnetized strip makes the amorphous strip respond much more strongly to the detectors, because the DC magnetic field given off by the strip offsets the magnetic anisotropy within the amorphous metal.
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Krishnan, along with other rising scientists such as Santilal ( S . ) Banerjee, B . C . Guha, and Asutosh Mookerjie developed an elegant and precise experimental technique to measure the magnetic anisotropy of dia and paramagnetic crystals.
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Theoretical computations showed approximately two magnetic electrons are localized on each Fe atom with the other atoms being nearly nonmagnetic, and the spin-orbit coupling potential energy surface has three local energy minima with a magnetic anisotropy barrier just below 3 meV.
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Commercial magnets are made of " hard " ferromagnetic or ferrimagnetic materials with very large magnetic anisotropy such as alnico and ferrites, which have a very strong tendency for the magnetization to be pointed along one axis of the crystal, the " easy axis ".
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