| 释义 |
- References
- Further reading
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 1. ^{{cite book |last = Chikazumi |first = Sōshin |title = Physics of Ferromagnetism |publisher = Clarendon Press |date = 1997 |isbn = 978-0-19-851776-4}}
Further reading{{Refbegin}}- {{cite journal|last=Beck|first=Paul A.|title=Comments on mictomagnetism|journal=Journal of the Less Common Metals|year=1972|volume=28|issue=1|pages=193–199|doi=10.1016/0022-5088(72)90180-4}}
- {{cite journal|last=Shull|first=R.D.|author2=Okamoto, H. |author3=Beck, P.A. |title=Transition from ferromagnetism to mictomagnetism in Fe—Al alloys|journal=Solid State Communications|year=1976|volume=20|issue=9|pages=863–868|doi=10.1016/0038-1098(76)91292-8|bibcode = 1976SSCom..20..863S }}
- {{cite book|last1=White|first1=Robert M.|title=Quantum Theory of Magnetism|date=1983|publisher=Springer Berlin Heidelberg|location=Berlin, Heidelberg|isbn=9783662023600|pages=245–246|edition=Second corrected and Updated}}
{{Refend}}{{electromagnetism-stub}}{{magnetic states}} 3 : Quantum phases|Magnetic ordering|Magnetic alloys |