Mictomagnetism
Mictomagnetism is a spin system in which various exchange interactions are mixed. It is observed in several kinds of alloys, including Cu–Mn, Fe–Al and Ni–Mn alloys. Cooled in zero magnetic field, these materials have low remanence and coercivity. Cooled in a magnetic field, they have much larger remanence, and the hysteresis loop is shifted in the direction opposite to the field (an effect similar to exchange bias).[1]
References
- ^ Chikazumi, Sōshin (1997). Physics of Ferromagnetism. Clarendon Press. ISBN 978-0-19-851776-4.
Further reading
- Beck, Paul A. (1972). "Comments on mictomagnetism". Journal of the Less Common Metals. 28 (1): 193–199. doi:10.1016/0022-5088(72)90180-4.
- Shull, R.D.; Okamoto, H.; Beck, P.A. (1976). "Transition from ferromagnetism to mictomagnetism in Fe—Al alloys". Solid State Communications. 20 (9): 863–868. Bibcode:1976SSCom..20..863S. doi:10.1016/0038-1098(76)91292-8.
- White, Robert M. (1983). Quantum Theory of Magnetism (Second corrected and Updated ed.). Berlin, Heidelberg: Springer Berlin Heidelberg. pp. 245–246. ISBN 9783662023600.
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Magnetism
- diamagnetism
- superdiamagnetism
- paramagnetism
- superparamagnetism
- Van Vleck paramagnetism
- altermagnetism
- antiferromagnetism
- ferrimagnetism
- ferromagnetism
- superferromagnetism
- ferromagnetic superconductor
- helimagnetism
- metamagnetism
- mictomagnetism
- spin glass
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