Exchange bias or exchange anisotropy occurs in bilayers (or multilayers) of magnetic materials where the hard magnetization behavior of an
antiferromagneticthin film causes a shift in the soft magnetization curve of a ferromagneticfilm. The exchange bias phenomenon is of tremendous utility in magnetic recording, where it is used to pin the state of the readback heads of hard diskdrives at exactly their point of maximum sensitivity; hence the term "bias."
The essential physics underlying the phenomenon is the exchange interaction between the antiferromagnet and ferromagnet at their interface. Since antiferromagnets have a small or no net magnetization, their spin orientation is only weakly influenced by an externally applied magnetic field. A soft ferromagnetic film which is strongly exchange-coupled to the antiferromagnet will have its interfacial spins pinned. Reversal of the ferromagnet's moment will have an added energetic cost corresponding to the energy necessary to create a Néel
domain wallwithin the ferromagnetic film. The added energy term implies a shift in the switching field of the ferromagnet. Thus the magnetization curve of an exchange-biased ferromagnetic film looks like that of the normal ferromagnet except that is shifted away from the H=0 axis by an amount Hb.
In most well-studied ferromagnet/antiferromagnet bilayers, the
Curie temperatureof the ferromagnet is larger than the Néel temperatureTN of the antiferromagnet. This inequality means that the direction of the exchange bias can be set by cooling through TN in the presence of an applied magnetic field. The moment of the magnetically ordered ferromagnet will apply an effective field to the antiferromagnet as it orders, breaking the symmetry and influencing the formation of domains.
anisotropyhas long been poorly understood due to the difficulty of studying the dynamics of domain walls in thin antiferromagnetic films. A naive approach to the problem would suggest the following expression for energy per unit area:
where "n" is the number of interfacial spins interactions per unit area, Jex is the exchange constant at the interface, S refers to the spin vector, M refers to the magnetization, t refers to film thickness and H is the external field. The subscript F describes the properties of the ferromagnet and AF to the antiferromagnet. The expression omits magnetocrystalline anisotropy, which is unaffected by the presence of the antiferromagnet. At the switching field of the ferromagnet, the pinning energy represented by the first term and the Zeeman dipole coupling represented by the second term will exactly balance. The equation then predicts that the exchange bias shift Hb will be given by the expression
Many experimental findings regarding the exchange bias contradict this simple model. For example, the magnitude of measured Hb values is typically 100 times less than that predicted by the equation for reasonable values of the parameters. The amount of hysteresis shift Hb is not correlated with the density "n" of uncompensated spins in the plane of the antiferromagnet that appears at the interface. In addition, the exchange bias effect tends to be smaller in epitaxial bilayers than in polycrystalline ones, suggesting an important role for defects. In recent years progress in fundamental understanding has been made via
synchrotronelement-specific magnetic linear dichroismexperiments that can image antiferromagnetic domains and frequency-dependent magnetic susceptibilitymeasurements that can probe the dynamics. Experiments on the Fe/FeF2 and Fe/MnF2 model systems have been particularly fruitful.
Exchange bias was initially used to stabilize the magnetization of soft ferromagnetic layers in readback heads based on the anisotropic
magnetoresistance(AMR) effect. Without the stabilization, the magnetic domain state of the head could be unpredictable, leading to reliability problems. Currently exchange bias is used to pin the harder reference layer in spin valvereadback heads and MRAMmemory circuits that utilize the giant magnetoresistanceor magnetic tunneling effect. Similarly the most advanced disk media are antiferromagnetically coupled, making use of interfacial exchange to effectively increase the stability of small magnetic particles whose behavior would otherwise be superparamagnetic.
Desirable properties for an exchange bias material include a high
Néel temperature, a large magnetocrystalline anisotropyand good chemical and structural compatibility with NiFe and Co, the most important ferromagnetic films. The most technologically significant exchange bias materials have been the rocksalt-structure antiferromagnetic oxides like NiO, CoO and their alloys and the rocksalt-structure intermetallics like FeMn, NiMn, IrMn and their alloys.
Exchange anisotropy was discovered by Meiklejohn and Bean of
General Electricin 1957. The first commercial device to employ the exchange bias was IBM's anisotropic magnetoresistance (AMR) disk drive recording head, which was based on a design by Hunt in the 1970s but which didn't fully displace the inductive readback head until the early 1990s. By the mid-1990s, the spin valvehead using an exchange-bias layer was well on its way to displacing the AMR head.
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title=New Magnetic Anisotropy
* S. Chikazumi and S.H. Charap, "Physics of Magnetism," ASIN B0007DODNA.
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doi = 10.1016/S0304-8853(98)00266-2
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issue = 2
pages = 203-232
last = Nogués
first = J.
Ivan K. Schuller
title = Exchange bias
journal = Journal of Magnetism and Magnetic Materials
date = 1999-02-15
* A.E. Berkowitz and K. Takano, [http://www2.hmc.edu/~eckert/research/berk.pdf "Exchange anisotropy: a review,"] J. Magn. Magn. Matls. 200, 552 (1999).
* John C. Mallinson, "Magneto-Resistive and Spin Valve Heads: Fundamentals and Applications," ISBN 0-12-466627-2.
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doi = 10.1016/S0304-8853(01)00421-8
volume = 234
issue = 3
pages = 584-595
last = Kiwi
first = Miguel
title = Exchange bias theory
journal = Journal of Magnetism and Magnetic Materials
date = 2001-09
Ivan K. Schullerand G. Guntherodt, [http://physics.ucsd.edu/~iksgrp/EBManifesto.pdf "The Exchange Bias Manifesto,"] 2002.
Jung-Il Hong, Titus Leo, David J. Smith, and Ami E. Berkowitz, [http://www.public.asu.edu/~tleo1/files/Hong_Titus_Leo_Smith_Berkowitz_Exchange_Bias.pdf "Enhancing Exchange Bias with Diluted Antiferromagnets,"] Phys. Rev. Lett. 96, 117204 (2006).
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