English subtitles for clip: File:Magnetic orders.webm

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Magnetic orders

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In some materials, atoms carry spins

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which are small quantum magnets
due to some of their electrons.

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In ferromagnets, the spins interact
with their neighbors and align.

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At low temperature, all the spins
are aligned over great distances.

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This is ferromagnetic order.

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The material then
exhibits a magnetization.

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[Ferromagnetism]

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But there are other magnetic orders.

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For example, spins sometimes prefer
to be anti-aligned with their neighbors.

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Here too, a long range order appears.
It's antiferromagnet.

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Yet the total magnetization remains zero.

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[Antiferromagnetism]

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There are even more subtle orders.

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For example,
two types of atom can alternate,

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one with a larger spin than the other.

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A ferrimagnetic order then appears.

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[Ferrimagnetism]

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Finally, in some cases, the situation
can be completely random.

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Imagine a ferromagnet.

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Then, suppose that, randomly,
some links are antiferromagnetic instead.

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Spins can no longer
all align or anti-align.

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They are frozen
but in a random configuration.

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It's a spin glass.

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When these different systems are heated,
they remain rigid up to a certain temperature.

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At the critical temperature Tc,
all the spins undergo a phase transition,

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like water boiling at 100 °C.

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The materials then suddenly lose
their order and become paramagnetic again.