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Usually refers to transition metal ions with unpaired electrons in 3d, 4d, or 5d shell in periods IV, V, and VIwhich give rise to paramagnetism and ferromagnetism.
In solids at sufficiently high temperatures, magnetic ions give rise to paramagnetism. The spins in a paramagnetic material align i. The total magnetic induction B is therefore larger than the applied field H.
This behavior is essentially the sum of the behaviors of the individual atoms, acting more-or-less independently. At low temperatures, a qualitatively different magnetic behavior occurs, which involves a collective interaction of the atoms: As a result, there is a spontaneous magnetization M, representing the self-consistent parallel orientation of atomic spins.
In large samples, the behavior is complicated by the interactions among different domains, and hysteresis history or memory effects occur. There is a qualitative contrast between induced-field effects in magnetism and electricity: The fundamental reason for this is in the sign of the force between similar elements: Other kinds of behavior occur, although metals with high magnetic-ion concentrations eventually at low enough temperature exhibit ferromagnetism.
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