Magnetic Oxides pp 37-106 | Cite as
Magnetic Ions in Oxides
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Abstract
To establish the pattern of this book, a logical first step is to review the Periodic table of chemical elements, to identify the transition groups within it, and to explain the local influences of the chemical bonding environment in which the various ions reside in a crystal lattice of an oxide. By the terminology of transition groups is meant those elements for which the inner shells remain unfilled while electrons occupying outer shells participate in chemical bonding. Consequently, the electrons of the unfilled inner shells are responsible for a variety of magnetic properties because of the magnetic moments carried by their unpaired spins.
From the theory of atomic spectra, the angular momentum of the electron spin is coupled to the angular momentum that is derived from the motion of the electron in its orbit about the nucleus, that is, the orbital angular momentum. The strength of spin–orbit coupling is a key factor in determining the extent to which the orbital moment contributes to the magnetic properties and conversely, to what extent the spins interact with the lattice. When placed in a crystal lattice, the magnetic ion is subjected to two effective fields that separately influence the spin and orbital momenta – the crystal electric field of the lattice site that captures or “quenches” the orbital moment by a Stark effect, and the exchange interaction that orders the spin into a collective ferromagnetic or antiferromagnetic state. The origin of the crystal and exchange fields is reviewed first. The role of spin–orbit coupling is examined later in relation to magnetocrystalline anisotropy and magnetostriction.
Keywords
Crystal Field Octahedral Site Orbital Angular Momentum Orbit Coupling Orbital StateReferences
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